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We search for an axion-like particle (ALP) a through the process ψ(3686)→π+π−J/ψ, J/ψ→γa, a→γγ in a data sample of (2.71±0.01)×109 ψ(3686) events collected by the BESIII detector. No significant ALP signal is observed over the expected background, and the upper limits on the branching fraction of the decay J/ψ→γa and the ALP-photon coupling constant gaγγ are set at 95% confidence level in the mass range of 0.165≤ma≤2.84GeV/c2. The limits on B(J/ψ→γa) range from 8.3×10−8 to 1.8×10−6 over the search region, and the constraints on the ALP-photon coupling are the most stringent to date for 0.165 ≤ ma ≤ 1.468GeV/c2.
Utilizing the data set corresponding to an integrated luminosity of 3.19 fb−1 collected by the BESIII detector at a center-of-mass energy of 4.178 GeV, we perform an amplitude analysis of the D+s→π+π−π+ decay. The sample contains 13,797 candidate events with a signal purity of ∼80%. We use a quasi-model-independent approach to measure the magnitude and phase of the D+s→π+π−π+ decay, where the P and D waves are parameterized by a sum of three Breit-Wigner amplitudes ρ(770)0, ρ(1450)0, and f2(1270). The fit fractions of different decay channels are also reported.
Utilizing the data set corresponding to an integrated luminosity of 3.19 fb−1 collected by the BESIII detector at a center-of-mass energy of 4.178 GeV, we perform an amplitude analysis of the D+s→π+π−π+ decay. The sample contains 13,797 candidates with a signal purity of ∼80%. The amplitude and phase of the contributing ππ S wave are measured based on a quasi-model-independent approach, along with the amplitudes and phases of the P and D waves parametrized by Breit-Wigner models. The fit fractions of different intermediate decay channels are also reported.
We report a measurement of the observed cross sections of e+ e− → J/ψX based on 3.21 fb − 1 of data accumulated at energies from 3.645 to 3.891 GeV with the BESIII detector operated at the BEPCII collider. In analysis of the cross sections, we measured the decay branching fractions of B(ψ(3686) → J/ψX) = (64.4 ± 0.6 ± 1.6)% and B(ψ(3770) → J/ψX) = (0.5 ± 0.2 ± 0.1)% for the first time. The energy-dependent line shape of these cross sections cannot be well described by two Breit-Wigner (BW) amplitudes of the expected decays ψ (3686) → J/ψX and ψ(3770) → J/ψX. Instead, it can be better described with one more BW amplitude of the decay R(3760)→ J/ψX. Under this assumption, we extracted the R (3760) mass M R (3760 ) = 3766.2 ± 3.8 ± 0.4 MeV/c2, total width Γ tot R ( 3760 ) = 22.2 ± 5.9 ± 1.4 MeV, and product of leptonic width and decay branching fraction
ΓeeR(3760) B[R(3760) → J/ψX] = (79.4 ± 85.5 ± 11.7) eV. The significance of the R(3760) is 5.3σ. The first uncertainties of these measured quantities are from fits to the cross sections and second systematic.
Measurement of cross sections for e⁺e⁻ → μ⁺μ⁻ at center-of-mass energies from 3.80 to 4.60 GeV
(2020)
The observed cross sections for 𝑒+𝑒−→𝜇+𝜇− at energies from 3.8 to 4.6 GeV are measured using data samples taken with the BESIII detector operated at the BEPCII collider. We measure the muonic widths and determine the branching fractions of the charmonium states 𝜓(4040), 𝜓(4160), and 𝜓(4415) decaying to 𝜇+𝜇−, as well as making a first determination of the phase of the amplitudes. In addition, we observe evidence for a structure in the dimuon cross section near 4.220 GeV/𝑐2, which we denote as 𝑆(4220). Analyzing a coherent sum of amplitudes yields eight solutions, one of which gives a mass of 𝑀𝑆(4220) = 4216.7±8.9±4.1 MeV/𝑐2, a total width of Γtot S(4220) = 47.2±22.8±10.5 MeV, and a muonic width of Γ𝜇𝜇 𝑆(4220) = 1.53±1.26±0.54 keV, where the first uncertainties are statistical and the second systematic. The eight solutions give the central values of the mass, total width, muonic width to be, respectively, in the range from 4212.8 to 4219.4 MeV/𝑐2, from 36.4 to 49.6 MeV, and from 1.09 to 1.53 keV. The statistical significance of the 𝑆(4220) signal is 3.9𝜎. Correcting the total dimuon cross section for radiative effects yields a statistical significance for this structure of 8.1𝜎.
We report on the first search for ¯Λ−Λ oscillations in the decay 𝐽/𝜓→𝑝𝐾−¯Λ+c.c. by analyzing 1.31×109 𝐽/𝜓 events accumulated with the BESIII detector at the BEPCII collider. The 𝐽/𝜓 events are produced using 𝑒+𝑒− collisions at a center of mass energy √𝑠=3.097 GeV. No evidence for hyperon oscillations is observed. The upper limit for the oscillation rate of ¯Λ to Λ hyperons is determined to be 𝒫(Λ)=[ℬ(𝐽/𝜓→𝑝𝐾−Λ+c.c.)/ℬ(𝐽/𝜓→𝑝𝐾−¯Λ+c.c.)]<4.4×10−6 corresponding to an oscillation parameter 𝛿𝑚Λ¯Λ of less than 3.8×10−18 GeV at the 90% confidence level.
There has recently been a dramatic renewal of interest in hadron spectroscopy and charm physics. This renaissance has been driven in part by the discovery of a plethora of charmonium-like XYZ states at BESIII and B factories, and the observation of an intriguing proton-antiproton threshold enhancement and the possibly related X(1835) meson state at BESIII, as well as the threshold measurements of charm mesons and charm baryons.
We present a detailed survey of the important topics in tau-charm physics and hadron physics that can be further explored at BESIII during the remaining operation period of BEPCII. This survey will help in the optimization of the data-taking plan over the coming years, and provides physics motivation for the possible upgrade of BEPCII to higher luminosity.
Search for the reaction channel e⁺e⁻ → ηcηπ⁺π⁻ at center-of-mass energies from 4.23 to 4.60 GeV
(2021)
Using data collected with the BESIII detector operating at the Beijing Electron Positron Collider, we search for the process 𝑒+𝑒−→𝜂𝑐𝜂𝜋+𝜋−. The search is performed using five large datasets recorded at center-of-mass energies of 4.23, 4.26, 4.36, 4.42, and 4.60 GeV. The 𝜂𝑐 meson is reconstructed in 16 exclusive decay modes. No signal is observed in the 𝜂𝑐 mass region at any center-of-mass energy. The upper limits on the reaction cross sections are determined to be 6.2, 10.8, 27.6, 22.6 and 23.7 pb at the 90% confidence level at the center-of-mass energies listed above.
Measurement of branching fractions for D meson decaying into ϕ meson and a pseudoscalar meson
(2019)
The four decay modes D0 → φπ0, D0 → φη, D+ → φπ+, and D+ → φK + are studied by using a data sample taken at the centre-of-mass energy √s = 3.773 GeV with the BESIII detector, corresponding to an integrated luminosity of 2.93 fb−1. The branching fractions of the first three decay modes are measured to be B(D0 → φπ0) = (1.168 ± 0.028 ± 0.028) × 10−3, B(D0 → φη) = (1.81 ± 0.46 ± 0.06) × 10−4, and B(D+ → φπ+) = (5.70 ± 0.05 ± 0.13) × 10−3, respectively, where the first uncertainties are statistical and the second are systematic. In addition, the upper limit of the branching fraction for D+ → φK+ is given to be 2.1 × 10−5 at the 90% confidence level. The ratio of B(D0 → φπ0) to B(D+ → φπ+) is calculated to be (20.49 ± 0.50 ± 0.45)%, which is consistent with the theoretical prediction based on isospin symmetry between these two decay modes.
The process 𝑒+𝑒−→𝜙𝜂′ has been studied for the first time in detail using data sample collected with the BESIII detector at the BEPCII collider at center of mass energies from 2.05 to 3.08 GeV. A resonance with quantum numbers 𝐽𝑃𝐶=1−− is observed with mass 𝑀=(2177.5±4.8(stat)±19.5(syst))MeV/𝑐2 and width Γ=(149.0±15.6(stat)±8.9(syst)) MeV with a statistical significance larger than 10𝜎, including systematic uncertainties. If the observed structure is identified with the 𝜙(2170), then the ratio of partial width between the 𝜙𝜂′ by BESIII and 𝜙𝜂 by BABAR is (ℬ𝑅𝜙𝜂Γ𝑅𝑒𝑒)/(ℬ𝑅𝜙𝜂′Γ𝑅𝑒𝑒)=0.23±0.10(stat)±0.18(syst), which is smaller than the prediction of the 𝑠¯𝑠𝑔 hybrid models by several orders of magnitude.
Using a low background data sample of 9.7×105 𝐽/𝜓→𝛾𝜂′, 𝜂′→𝛾𝜋+𝜋− events, which are 2 orders of magnitude larger than those from the previous experiments, recorded with the BESIII detector at BEPCII, the decay dynamics of 𝜂′→𝛾𝜋+𝜋− are studied with both model-dependent and model-independent approaches. The contributions of 𝜔 and the 𝜌(770)−𝜔 interference are observed for the first time in the decays 𝜂′→𝛾𝜋+𝜋− in both approaches. Additionally, a contribution from the box anomaly or the 𝜌(1450) resonance is required in the model-dependent approach, while the process specific part of the decay amplitude is determined in the model-independent approach.
A partial-wave analysis of the decay 𝐽/𝜓→𝐾+𝐾−𝜋0 has been made using (223.7±1.4)×106 𝐽/𝜓 events collected with the BESIII detector in 2009. The analysis, which is performed within the isobar-model approach, reveals contributions from 𝐾*2(1430)±, 𝐾*2(1980)± and 𝐾*4(2045)± decaying to 𝐾±𝜋0. The two latter states are observed in 𝐽/𝜓 decays for the first time. Two resonance signals decaying to 𝐾+𝐾− are also observed. These contributions cannot be reliably identified and their possible interpretations are discussed. The measured branching fraction 𝐵(𝐽/𝜓→𝐾+𝐾−𝜋0) of (2.88±0.01±0.12)×10−3 is more precise than previous results. Branching fractions for the reported contributions are presented as well. The results of the partial-wave analysis differ significantly from those previously obtained by BESII and BABAR.
We measure the Born cross sections of the process 𝑒+𝑒−→𝐾+𝐾−𝐾+𝐾− at center-of-mass (c.m.) energies, √𝑠, between 2.100 and 3.080 GeV. The data were collected using the BESIII detector at the BEPCII collider. An enhancement at √𝑠=2.232 GeV is observed, very close to the 𝑒+𝑒−→Λ¯Λ production threshold. A similar enhancement at the same c.m. energy is observed in the 𝑒+𝑒−→𝜙𝐾+𝐾− cross section. The energy dependence of the 𝐾+𝐾−𝐾+𝐾− and 𝜙𝐾+𝐾− cross sections differs significantly from that of 𝑒+𝑒−→𝜙𝜋+𝜋−.
Using 𝑒+𝑒−→Λ+𝑐¯Λ−𝑐 production from a 567 pb−1 data sample collected by BESIII at 4.6 GeV, a full angular analysis is carried out simultaneously on the four decay modes of Λ+𝑐→𝑝𝐾0𝑆, Λ𝜋+, Σ+𝜋0, and Σ0𝜋+. For the first time, the Λ+𝑐 transverse polarization is studied in unpolarized 𝑒+𝑒− collisions, where a nonzero effect is observed with a statistical significance of 2.1𝜎. The decay asymmetry parameters of the Λ+𝑐 weak hadronic decays into 𝑝𝐾0𝑆, Λ𝜋+, Σ+𝜋0 and Σ0𝜋+ are measured to be 0.18±0.43(stat)±0.14(syst), −0.80±0.11(stat)±0.02(syst), −0.57±0.10(stat)±0.07(syst), and −0.73±0.17(stat)±0.07(syst), respectively. In comparison with previous results, the measurements for the Λ𝜋+ and Σ+𝜋0 modes are consistent but with improved precision, while the parameters for the 𝑝𝐾0𝑆 and Σ0𝜋+ modes are measured for the first time.
By analyzing the large-angle Bhabha scattering events e+e− → (γ)e+e− and diphoton events e+e− → (γ)γγ for the data sets collected at center-of-mass (c.m.) energies between 2.2324 and 4.5900 GeV (131 energy points in total) with the upgraded Beijing Spectrometer (BESIII) at the Beijing Electron-Positron Collider (BEPCII), the integrated luminosities have been measured at the different c.m. energies, individually. The results are important inputs for the R value and J/ψ resonance parameter measurements.
We study the decays of J/ψ and ψ(3686) to the final states Σ(1385)0Σ¯(1385)0 and Ξ0Ξ¯0 based on a single baryon tag method using data samples of (1310.6±7.0)×106 J/ψ and (447.9±2.9)×106 ψ(3686) events collected with the BESIII detector at the BEPCII collider. The decays to Σ(1385)0Σ¯(1385)0 are observed for the first time. The measured branching fractions of J/ψ and ψ(3686)→Ξ0Ξ¯0 are in good agreement with, and much more precise, than the previously published results. The angular parameters for these decays are also measured for the first time. The measured angular decay parameter for J/ψ→Σ(1385)0Σ¯(1385)0, α=−0.64±0.03±0.10, is found to be negative, different to the other decay processes in this measurement. In addition, the "12\% rule" and isospin symmetry in the J/ψ and ψ(3686)→ΞΞ¯ and Σ(1385)Σ¯(1385) systems are tested.
By analyzing 2.93 fb−1 of data taken at the ψ(3770) resonance peak with the BESIII detector, we measure the branching fractions for the hadronic decays D+ → K0S K0S K +, D+ → K0S K0Sπ+, D0 → K0S K0S and D0 → K0S K0S K0S . They are determined to be B(D+ → K0S K0S K +) = (2.54 ± 0.05stat. ± 0.12sys.) × 10−3, B(D+ → K0S K0Sπ+) = (2.70 ± 0.05stat. ± 0.12sys.) × 10−3, B(D0 → K0S K0S ) = (1.67 ± 0.11stat. ± 0.11sys.) × 10−4 and B(D0 → K0S K0S K0S ) = (7.21 ± 0.33stat. ± 0.44sys.) × 10−4, where the second one is measured for the first time and the others are measured with significantly improved precision over the previous measurements.
The decays of χc2→K+K−π0, KSK±π∓ and π+π−π0 are studied with the ψ(3686) data samples collected with the Beijing Spectrometer (BESIII). For the first time, the branching fractions of χc2→K∗K¯¯¯¯¯, χc2→a±2(1320)π∓/a02(1320)π0 and χc2→ρ(770)±π∓ are measured. Here K∗K¯¯¯¯¯ denotes both K∗±K∓ and K∗0K¯¯¯¯¯0+c.c., and K∗ denotes the resonances K∗(892), K∗2(1430) and K∗3(1780). The observations indicate a strong violation of the helicity selection rule in χc2 decays into vector and pseudoscalar meson pairs. The measured branching fractions of χc2→K∗(892)K¯¯¯¯¯ are more than 10 times larger than the upper limit of χc2→ρ(770)±π∓, which is so far the first direct observation of a significant U-spin symmetry breaking effect in charmonium decays.
Using data samples collected with the BESIII detector at the BEPCII collider at six center-of-mass energies between 4.008 and 4.600 GeV, we observe the processes e+e− → φφω and e+e− → φφφ. The Born cross sections are measured and the ratio of the cross sections σ(e+e− → φφω)/σ(e+e− → φφφ) is estimated to be 1.75 ± 0.22 ± 0.19 averaged over six energy points, where the first uncertainty is statistical and the second is systematic. The results represent first measurements of these interactions.
Measurements of cross section of e⁺e⁻ → pp¯π⁰ at center-of-mass energies between 4.008 and 4.600 GeV
(2017)
Based on e+e− annihilation data samples collected with the BESIII detector at the BEPCII collider at 13 center-of-mass energies from 4.008 to 4.600 GeV, measurements of the Born cross section of e+e− → pp¯π0 are performed. No significant resonant structure is observed in the measured energy dependence of the cross section. The upper limit on the Born cross section of e+e− → Y (4260) → pp¯π0 at the 90% C.L. is determined to be 0.01 pb. The upper limit on the ratio of the branching fractions B(Y (4260)→pp¯π0) B(Y (4260)→π+π− J/ψ) at the 90% C.L. is determined to be 0.02%.
The decays of χc2→K+K−π0, KSK±π∓ and π+π−π0 are studied with the ψ(3686) data samples collected with the Beijing Spectrometer (BESIII). For the first time, the branching fractions of χc2→K∗K¯¯¯¯¯, χc2→a±2(1320)π∓/a02(1320)π0 and χc2→ρ(770)±π∓ are measured. Here K∗K¯¯¯¯¯ denotes both K∗±K∓ and K∗0K¯¯¯¯¯0+c.c., and K∗ denotes the resonances K∗(892), K∗2(1430) and K∗3(1780). The observations indicate a strong violation of the helicity selection rule in χc2 decays into vector and pseudoscalar meson pairs. The measured branching fractions of χc2→K∗(892)K¯¯¯¯¯ are more than 20 times larger than that of χc2→ρ(770)±π∓, which implies the effects are largely due to U-spin symmetry breaking, rather than just isospin symmetry breaking in charmonium decays.
The decays of χc2→K+K−π0, KSK±π∓ and π+π−π0 are studied with the ψ(3686) data samples collected with the Beijing Spectrometer (BESIII). For the first time, the branching fractions of χc2→K∗K¯¯¯¯¯, χc2→a±2(1320)π∓/a02(1320)π0 and χc2→ρ(770)±π∓ are measured. Here K∗K¯¯¯¯¯ denotes both K∗±K∓ and K∗0K¯¯¯¯¯0+c.c., and K∗ denotes the resonances K∗(892), K∗2(1430) and K∗3(1780). The observations indicate a strong violation of the helicity selection rule in χc2 decays into vector and pseudoscalar meson pairs. The measured branching fractions of χc2→K∗(892)K¯¯¯¯¯ are more than 20 times larger than that of χc2→ρ(770)±π∓, which implies the effects are largely due to U-spin symmetry breaking, rather than just isospin symmetry breaking in charmonium decays.
The decays of χc2→K+K−π0, KSK±π∓ and π+π−π0 are studied with the ψ(3686) data samples collected with the Beijing Spectrometer (BESIII). For the first time, the branching fractions of χc2→K∗K¯¯¯¯¯, χc2→a±2(1320)π∓/a02(1320)π0 and χc2→ρ(770)±π∓ are measured. Here K∗K¯¯¯¯¯ denotes both K∗±K∓ and K∗0K¯¯¯¯¯0+c.c., and K∗ denotes the resonances K∗(892), K∗2(1430) and K∗3(1780). The observations indicate a strong violation of the helicity selection rule in χc2 decays into vector and pseudoscalar meson pairs. The measured branching fractions of χc2→K∗(892)K¯¯¯¯¯ are more than 10 times larger than the upper limit of χc2→ρ(770)±π∓, which is so far the first direct observation of a significant U-spin symmetry breaking effect in charmonium decays.
Using an 𝑒+𝑒− collision data sample of 2.93 fb−1 collected at a center-of-mass energy of 3.773 GeV by the BESIII detector at BEPCII, we report the observation of 𝐷0→𝑎0(980)−𝑒+𝜈𝑒 and evidence for 𝐷+→𝑎0(980)0𝑒+𝜈𝑒 with significances of 6.4𝜎 and 2.9𝜎, respectively. The absolute branching fractions are determined to be ℬ(𝐷0→𝑎0(980)−𝑒+𝜈𝑒)×ℬ(𝑎0(980)−→𝜂𝜋−) = [1.33+0.33−0.29(stat)±0.09(syst)]×10−4 and ℬ(𝐷+→𝑎0(980)0𝑒+𝜈𝑒)×ℬ(𝑎0(980)0→𝜂𝜋0)=[1.66+0.81
−0.66(stat)±0.11(syst)]×10−4. This is the first time the 𝑎0(980) meson has been measured in a 𝐷0 semileptonic decay, which would open one more interesting page in the investigation of the nature of the puzzling 𝑎0(980) states.
The cross section of the process e+e−→K+K− is measured at a number of center-of-mass energies s√ from 2.00 to 3.08 GeV with the BESIII detector at the Beijing Electron Positron Collider (BEPCII). The results provide the best precision achieved so far. A resonant structure around 2.2 GeV is observed in the cross section line shape. A Breit-Wigner fit yields a mass of M=2239.2±7.1±11.3~and a width of Γ=139.8±12.3±20.6 MeV, where the first uncertainties are statistical and the second ones are systematic. In addition, the time-like electromagnetic form factor of the kaon is determined at the individual center-of-mass energy points.
Using a 3.19 fb−1 data sample collected at an 𝑒+𝑒− center-of-mass energy of 𝐸cm=4.178 GeV with the BESIII detector, we measure the branching fraction of the leptonic decay 𝐷+𝑠→𝜇+𝜈𝜇 to be ℬ𝐷+𝑠→𝜇+𝜈𝜇=(5.49±0.16stat±0.15syst)×10−3. Combining our branching fraction with the masses of the 𝐷+𝑠 and 𝜇+ and the lifetime of the 𝐷+𝑠, we determine 𝑓𝐷+𝑠|𝑉𝑐𝑠|=246.2±3.6stat±3.5syst MeV. Using the 𝑐→𝑠 quark mixing matrix element |𝑉𝑐𝑠| determined from a global standard model fit, we evaluate the 𝐷+𝑠 decay constant 𝑓𝐷+𝑠=252.9±3.7stat±3.6syst MeV. Alternatively, using the value of 𝑓𝐷+𝑠 calculated by lattice quantum chromodynamics, we find |𝑉𝑐𝑠|=0.985±0.014stat±0.014syst. These values of ℬ𝐷+𝑠→𝜇+𝜈𝜇, 𝑓𝐷+𝑠|𝑉𝑐𝑠|, 𝑓𝐷+𝑠 and |𝑉𝑐𝑠| are each the most precise results to date.
Using a data sample of 448.1×106 𝜓(3686) events collected at √𝑠=3.686 GeV with the BESIII detector at the Beijing Electron-Positron Collider II, we search for the rare decay 𝐽/𝜓→𝜙𝑒+𝑒− via 𝜓(3686)→𝜋+𝜋−𝐽/𝜓. No signal events are observed and the upper limit on the branching fraction is set to be ℬ(𝐽/𝜓→𝜙𝑒+𝑒−)<1.2×10−7 at the 90% confidence level, which is still about one order of magnitude higher than the Standard Model prediction.
he process e+e−→pK0Sn¯K−+c.c. and its intermediate processes are studied for the first time, using data samples collected with the BESIII detector at BEPCII at center-of-mass energies of 3.773, 4.008, 4.226, 4.258, 4.358, 4.416, and 4.600 GeV, with a total integrated luminosity of 7.4 fb−1. The Born cross section of e+e−→pK0Sn¯K−+c.c. is measured at each center-of-mass energy, but no significant resonant structure in the measured cross-section line shape between 3.773 and 4.600 GeV is observed. No evident structure is detected in the pK−, nK0S, pK0S, nK+, pn¯, or K0SK− invariant mass distributions except for Λ(1520). The Born cross sections of e+e−→Λ(1520)n¯K0S+c.c. and e+e−→Λ(1520)p¯K++c.c. are measured, and the 90\% confidence level upper limits on the Born cross sections of e+e−→Λ(1520)Λ¯(1520) are determined at the seven center-of-mass energies.
We report new measurements of the cross sections for the production of Dbar D final states at the ψ(3770) resonance. Our data sample consists of an integrated luminosity of 2.93 fb−1 of e+e− annihilation data produced by the BEPCII collider and collected and analyzed with the BESIII detector. We exclusively reconstruct three D0 and six D+ hadronic decay modes and use the ratio of the yield of fully reconstructed Dbar D events ("double tags") to the yield of all reconstructed D or bar D mesons ("single tags") to determine the number of D0bar D0 and D+D− events, benefiting from the cancellation of many systematic uncertainties. Combining these yields with an independent determination of the integrated luminosity of the data sample, we find the cross sections to be σ(e+e− → D0bar D0) nb and σ(e+e− → D+D−) = (2.830 ± 0.011 ± 0.026) nb, where the uncertainties are statistical and systematic, respectively.
We study the hadronic decays of Λ+c to the final states Σ+η and Σ+η′, using an e+e− annihilation data sample of 567 pb−1 taken at a center-of-mass energy of 4.6 GeV with the BESIII detector at the BEPCII collider. We find evidence for the decays Λ+c→Σ+η and Σ+η′ with statistical significance of 2.5σ and 3.2σ, respectively. Normalizing to the reference decays Λ+c→Σ+π0 and Σ+ω, we obtain the ratios of the branching fractions B(Λ+c→Σ+η)B(Λ+c→Σ+π0) and B(Λ+c→Σ+η′)B(Λ+c→Σ+ω) to be 0.35±0.16±0.03 and 0.86±0.34±0.07, respectively. The upper limits at the 90\% confidence level are set to be B(Λ+c→Σ+η)B(Λ+c→Σ+π0)<0.58 and B(Λ+c→Σ+η′)B(Λ+c→Σ+ω)<1.2. Using BESIII measurements of the branching fractions of the reference decays, we determine B(Λ+c→Σ+η)=(0.41±0.19±0.05)% (<0.68%) and B(Λ+c→Σ+η′)=(1.34±0.53±0.21)% (<1.9%). Here, the first uncertainties are statistical and the second systematic. The obtained branching fraction of Λ+c→Σ+η is consistent with the previous measurement, and the branching fraction of Λ+c→Σ+η′ is measured for the first time.
We study the electromagnetic Dalitz decay 𝐽/𝜓→𝑒+𝑒−𝜂 and search for dielectron decays of a dark gauge boson (𝛾′) in 𝐽/𝜓→𝛾′𝜂 with the two 𝜂 decay modes 𝜂→𝛾𝛾 and 𝜂→𝜋+𝜋−𝜋0 using (1310.6±7.0)×106 𝐽/𝜓 events collected with the BESIII detector. The branching fraction of 𝐽/𝜓→𝑒+𝑒−𝜂 is measured to be (1.43±0.04(stat)±0.06(syst))×10−5, with a precision that is improved by a factor of 1.5 over the previous BESIII measurement. The corresponding dielectron invariant mass dependent modulus square of the transition form factor is explored for the first time, and the pole mass is determined to be Λ=2.84±0.11(stat)±0.08(syst) GeV/𝑐2. We find no evidence of 𝛾′ production and set 90% confidence level upper limits on the product branching fraction ℬ(𝐽/𝜓→𝛾′𝜂)×ℬ(𝛾′→𝑒+𝑒−) as well as the kinetic mixing strength between the standard model photon and 𝛾′ in the mass range of 0.01≤𝑚𝛾′≤2.4 GeV/𝑐2.
Using a data sample of 448.1×106 ψ(3686) events collected at s√= 3.686 GeV with the BESIII detector at the BEPCII, we search for the rare decay J/ψ→ϕe+e− via ψ(3686)→π+π−J/ψ. No signal events are observed and the upper limit on the branching fraction is set to be B(J/ψ→ϕe+e−)<1.2×10−7 at the 90\% confidence level, which is still about one order of magnitude higher than the Standard Model prediction.
We report on new measurements of Cabibbo-suppressed semileptonic D+s decays using 3.19 fb−1 of e+e− annihilation data sample collected at a center-of-mass energy of 4.178~GeV with the BESIII detector at the BEPCII collider. Our results include branching fractions B(D+s→K0e+νe)=(3.25±0.38(stat.)±0.16(syst.))×10−3 and B(D+s→K∗0e+νe)=(2.37±0.26(stat.)±0.20(syst.))×10−3 which are much improved relative to previous measurements, and the first measurements of the hadronic form-factor parameters for these decays. For D+s→K0e+νe, we obtain f+(0)=0.720±0.084(stat.)±0.013(syst.), and for D+s→K∗0e+νe, we find form-factor ratios rV=V(0)/A1(0)=1.67±0.34(stat.)±0.16(syst.) and r2=A2(0)/A1(0)=0.77±0.28(stat.)±0.07(syst.).
Using a data sample with an integrated luminosity of 2.93 fb−1 taken at the center-of-mass energy of 3.773 GeV, we search for the Majorana neutrino (𝜈𝑚) in the lepton number violating decays 𝐷→𝐾𝜋𝑒+𝑒+. No significant signal is observed, and the upper limits on the branching fraction at the 90% confidence level are set to be ℬ(𝐷0→𝐾−𝜋−𝑒+𝑒+)<2.8×10−6, ℬ(𝐷+→𝐾0𝑆𝜋−𝑒+𝑒+)<3.3×10−6 and ℬ(𝐷+→𝐾−𝜋0𝑒+𝑒+)<8.5×10−6. The Majorana neutrino is searched for with different mass assumptions ranging from 0.25 to 1.0 GeV/𝑐2 in the decays 𝐷0→𝐾−𝑒+𝜈𝑚,𝜈𝑚→𝜋−𝑒+ and 𝐷+→𝐾0𝑆𝑒+𝜈𝑚,𝜈𝑚→𝜋−𝑒+, and the upper limits on the branching fraction at the 90% confidence level are at the level of 10−7∼10−6, depending on the mass of the Majorana neutrino. The constraints on the mixing matrix element |𝑉𝑒𝜈𝑚|2 are also evaluated.
We report the first measurement of the absolute branching fraction for Λ+c→Λμ+νμ. This measurement is based on a sample of e+e− annihilation data at a center-of-mass energy of s√=4.6 GeV collected with the BESIII detector at the BEPCII storage rings. The sample corresponds to an integrated luminosity of 567 pb−1. The branching fraction is determined to be B(Λ+c→Λμ+νμ)=(3.49±0.46(stat)±0.27(syst))%. In addition, we calculate the ratio B(Λ+c→Λμ+νμ)/B(Λ+c→Λe+νe) to be 0.96±0.16(stat)±0.04(syst).
Using a data sample of 448.1 × 106 ψ(3686) events collected with the BESIII detector at the BEPCII collider, we report the first observation of the electromagnetic Dalitz decay ψ(3686) → η e+e−, with significances of 7.0σ and 6.3σ when reconstructing the η meson via its decay modes η → γπ+π− and η → π+π−η (η → γγ ), respectively. The weighted average branching fraction is determined to be B(ψ(3686) → η e+e−) = (1.90 ± 0.25 ± 0.11) × 10−6, where the first uncertainty is statistical and the second systematic.
Using a sample of 106 million 𝜓(3686) decays, 𝜓(3686)→𝛾𝜒𝑐𝐽(𝐽=0,1,2) and 𝜓(3686)→𝛾𝜒𝑐𝐽,𝜒𝑐𝐽→𝛾𝐽/𝜓(𝐽=1,2) events are utilized to study inclusive 𝜒𝑐𝐽→anything, 𝜒𝑐𝐽→hadrons, and 𝐽/𝜓→anything distributions, including distributions of the number of charged tracks, electromagnetic calorimeter showers, and 𝜋0s, and to compare them with distributions obtained from the BESIII Monte Carlo simulation. Information from each Monte Carlo simulated decay event is used to construct matrices connecting the detected distributions to the input predetection “produced” distributions. Assuming these matrices also apply to data, they are used to predict the analogous produced distributions of the decay events. Using these, the charged particle multiplicities are compared with results from MARK I. Further, comparison of the distributions of the number of photons in data with those in Monte Carlo simulation indicates that G-parity conservation should be taken into consideration in the simulation.
We report the first observation of the semimuonic decay 𝐷+→𝜔𝜇+𝜈𝜇 using an 𝑒+𝑒− collision data sample corresponding to an integrated luminosity of 2.93 fb−1 collected with the BESIII detector at a center-of-mass energy of 3.773 GeV. The absolute branching fraction of the 𝐷+→𝜔𝜇+𝜈𝜇 decay is measured to be ℬ𝐷+→𝜔𝜇+𝜈𝜇=(17.7±1.8stat±1.1syst)×10−4. Its ratio with the world average value of the branching fraction of the 𝐷+→𝜔𝑒+𝜈𝑒 decay probes lepton flavor universality and it is determined to be ℬ𝐷+→𝜔𝜇+𝜈𝜇/ℬPDG 𝐷+→𝜔𝑒+𝜈𝑒=1.05±0.14, in agreement with the standard model expectation within one standard deviation.
Using a data sample of e+e− collision data corresponding to an integrated luminosity of 2.93 fb−1 collected with the BESIII detector at a center-of-mass energy of s=3.773GeV, we search for the singly Cabibbo-suppressed decays D0→π0π0π0, π0π0η, π0ηη and ηηη using the double tag method. The absolute branching fractions are measured to be B(D0→π0π0π0)=(2.0±0.4±0.3)×10−4, B(D0→π0π0η)=(3.8±1.1±0.7)×10−4 and B(D0→π0ηη)=(7.3±1.6±1.5)×10−4 with the statistical significances of 4.8σ, 3.8σ and 5.5σ, respectively, where the first uncertainties are statistical and the second ones systematic. No significant signal of D0→ηηη is found, and the upper limit on its decay branching fraction is set to be B(D0→ηηη)<1.3×10−4 at the 90% confidence level.
Using 16 energy points of e+e− annihilation data collected in the vicinity of the J/ψ resonance with the BESIII detector and with a total integrated luminosity of around 100 pb−1, we study the relative phase between the strong and electromagnetic amplitudes of J/ψ decays. The relative phase between J/ψ electromagnetic decay and the continuum process (e+e− annihilation without the J/ψ resonance) is confirmed to be zero by studying the cross section lineshape of μ+μ− production. The relative phase between J/ψ strong and electromagnetic decays is then measured to be (84.9 ± 3.6)◦ or (−84.7 ± 3.1)◦ for the 2(π+π−)π0 final state by investigating the interference pattern between the J/ψ decay and the continuum process. This is the first measurement of the relative phase between J/ψ strong and electromagnetic decays into a multihadron final state using the lineshape of the production cross section. We also study the production lineshape of the multihadron final state ηπ+π− with η → π+π−π0, which provides additional information about the phase between the J/ψ electromagnetic decay amplitude and the continuum process. Additionally, the branching fraction of J/ψ → 2(π+π−)π0 is measured to be (4.73 ± 0.44)% or (4.85 ± 0.45)%, and the branching fraction of J/ψ → ηπ+π− is measured to be (3.78 ± 0.68) × 10−4. Both of them are consistent with the world average values. The quoted uncertainties include both statistical and systematic uncertainties, which are mainly caused by the low statistics.
We report the first observation of the decay Λ+c→Σ−π+π+π0, based on data obtained in e+e− annihilations with an integrated luminosity of 567~pb−1 at s√=4.6~GeV. The data were collected with the BESIII detector at the BEPCII storage rings. The absolute branching fraction B(Λ+c→Σ−π+π+π0) is determined to be (2.11±0.33(stat.)±0.14(syst.))%. In addition, an improved measurement of B(Λ+c→Σ−π+π+) is determined as (1.81±0.17(stat.)±0.09(syst.))%.
We report the first measurements of absolute branching fractions for the W -exchange-only processes + c → 0K + and + c → (1530)0K + with the double-tag technique, by analyzing an e+e− collision data sample, that corresponds to an integrated luminosity of 567 pb−1 collected at a center-of-mass energy of 4.6 GeV by the BESIII detector. The branching fractions are measured to be B(+c → 0K +) = (5.90 ± 0.86 ± 0.39) × 10−3 and B(+c → (1530)0K +) = (5.02 ± 0.99 ± 0.31) × 10−3, where the first uncertainties are statistical and the second systematic. Our results are more precise than the previous relative measurements.
Measurement of the e+e−→π+π− cross section between 600 and 900 MeV using initial state radiation
(2016)
We extract the e+e− →π+π− cross section in the energy range between 600 and 900 MeV, exploiting the method of initial state radiation. A data set with an integrated luminosity of 2.93 fb−1 taken at a center-of-mass energy of 3.773 GeV with the BESIII detector at the BEPCII collider is used. The cross section is measured with a systematic uncertainty of 0.9%. We extract the pion form factor |Fπ|2 as well as the contribution of the measured cross section to the leading-order hadronic vacuum polarization contribution to (g−2)μ. We find this value to be aππ,LO μ (600–900 MeV) = (368.2 ±2.5stat±3.3sys) ·10−10, which is between the corresponding values using the BaBar or KLOE data.
An amplitude analysis of the 𝐾𝑆𝐾𝑆 system produced in radiative 𝐽/𝜓 decays is performed using the (1310.6±7.0)×106 𝐽/𝜓 decays collected by the BESIII detector. Two approaches are presented. A mass-dependent analysis is performed by parametrizing the 𝐾𝑆𝐾𝑆 invariant mass spectrum as a sum of Breit-Wigner line shapes. Additionally, a mass-independent analysis is performed to extract a piecewise function that describes the dynamics of the 𝐾𝑆𝐾𝑆 system while making minimal assumptions about the properties and number of poles in the amplitude. The dominant amplitudes in the mass-dependent analysis include the 𝑓0(1710), 𝑓0(2200), and 𝑓′2(1525). The mass-independent results, which are made available as input for further studies, are consistent with those of the mass-dependent analysis and are useful for a systematic study of hadronic interactions. The branching fraction of radiative 𝐽/𝜓 decays to 𝐾𝑆𝐾𝑆 is measured to be (8.1±0.4)×10−4, where the uncertainty is systematic and the statistical uncertainty is negligible.
Using a sample of 4.48×108 ψ(3686) events collected with the BESIII detector at the BEPCII collider, we study the two-photon decays of the pseudoscalar mesons π0, η, η′, η(1405), η(1475), η(1760), and X(1835) in J/ψ radiative decays using ψ(3686)→π+π−J/ψ events. The π0, η and η′ mesons are clearly observed in the two-photon mass spectra, and the branching fractions are determined to be B(J/ψ→γπ0→3γ)=(3.57±0.12±0.16)×10−5, B(J/ψ→γη→3γ)=(4.42±0.04±0.18)×10−4, and B(J/ψ→γη′→3γ)=(1.26±0.02±0.05)×10−4, where the first errors are statistical and the second systematic. No clear signal for η(1405), η(1475), η(1760) or X(1835) is observed in the two-photon mass spectra, and upper limits at the 90% confidence level on the product branching fractions are obtained.
Based on an 𝑒+𝑒− collision data sample corresponding to an integrated luminosity of 567 pb−1 taken at the center-of-mass energy of √𝑠=4.6 GeV with the BESIII detector, we measure the absolute branching fraction of the inclusive decay Λ+𝑐→Λ+𝑋 to be ℬ(Λ+𝑐→Λ+𝑋)=(38.2+2.8−2.2±0.9)% using the double-tag method, where 𝑋 refers to any possible final state particles. In addition, we search for direct 𝐶𝑃 violation in the charge asymmetry of this inclusive decay for the first time, and obtain 𝒜𝐶𝑃≡[ℬ(Λ+𝑐→Λ+𝑋)−ℬ(¯Λ−𝑐 → ¯Λ+𝑋)]/[ℬ(Λ+𝑐→Λ+𝑋)+ℬ(¯Λ−𝑐 → ¯Λ+𝑋)]=(2.1+7.0−6.6±1.6)%, a statistically limited result with no evidence of 𝐶𝑃 violation.
The decay 𝐽/𝜓→𝛾𝛾𝜙 is studied using a sample of 1.31×109 𝐽/𝜓 events collected with the BESIII detector. Two structures around 1475 MeV/𝑐2 and 1835 MeV/𝑐2 are observed in the 𝛾𝜙 invariant mass spectrum for the first time. With a fit on the 𝛾𝜙 invariant mass, which takes into account the interference between the two structures, and a simple analysis of the angular distribution, the structure around 1475 MeV/𝑐2 is found to favor an assignment as the 𝜂(1475) and the mass and width for the structure around 1835 MeV/𝑐2 are consistent with the 𝑋(1835). The statistical significances of the two structures are 13.5𝜎 and 6.3𝜎, respectively. The results indicate that both 𝜂(1475) and 𝑋(1835) contain a sizeable 𝑠¯𝑠 component.
Using a data sample of 𝑒+𝑒− collisions corresponding to an integrated luminosity of 567 pb−1 collected at a center-of-mass energy of √𝑠=4.6 GeV with the BESIII detector, we measure the absolute branching fraction of the inclusive semileptonic Λ+𝑐 decay with a double-tag method. We obtain ℬ(Λ+𝑐→𝑋𝑒+𝜈𝑒)=(3.95±0.34±0.09)%, where the first uncertainty is statistical and the second systematic. Using the known Λ+𝑐 lifetime and the charge-averaged semileptonic decay width of nonstrange charmed mesons (𝐷0 and 𝐷+), we obtain the ratio of the inclusive semileptonic decay widths Γ(Λ+𝑐→𝑋𝑒+𝜈𝑒)/¯Γ(𝐷→𝑋𝑒+𝜈𝑒)=1.26±0.12.
Using a data sample of 448.1×106 𝜓(3686) events collected with the BESIII detector operating at the BEPCII, we perform search for the hadronic transition ℎ𝑐→𝜋+𝜋−𝐽/𝜓 via 𝜓(3686)→𝜋0ℎ𝑐. No signals of the transition are observed, and the upper limit on the product branching fraction ℬ(𝜓(3686)→𝜋0ℎ𝑐)ℬ(ℎ𝑐→𝜋+𝜋−𝐽/𝜓) at the 90% confidence level (C.L.) is determined to be 2.0×10−6. This is the most stringent upper limit to date.
The polarization of Λ and Λ¯ hyperons along the beam direction has been measured relative to the second and third harmonic event planes in isobar Ru+Ru and Zr+Zr collisions at √sNN = 200 GeV. This is the first experimental evidence of the hyperon polarization by the triangular flow originating from the initial density fluctuations. The amplitudes of the sine modulation for the second and third harmonic results are comparable in magnitude, increase from central to peripheral collisions, and show a mild pT dependence. The azimuthal angle dependence of the polarization follows the vorticity pattern expected due to elliptic and triangular anisotropic flow, and qualitatively disagree with most hydrodynamic model calculations based on thermal vorticity and shear induced contributions. The model results based on one of existing implementations of the shear contribution lead to a correct azimuthal angle dependence, but predict centrality and pT dependence that still disagree with experimental measurements. Thus, our results provide stringent constraints on the thermal vorticity and shear-induced contributions to hyperon polarization. Comparison to previous measurements at RHIC and the LHC for the second-order harmonic results shows little dependence on the collision system size and collision energy.
J/ψ suppression has long been considered a sensitive signature of the formation of the Quark-Gluon Plasma (QGP) in relativistic heavy-ion collisions. In this letter, we present the first measurement of inclusive J/ψ production at mid-rapidity through the dimuon decay channel in Au+Au collisions at √sNN = 200 GeV with the STAR experiment. These measurements became possible after the installation of the Muon Telescope Detector was completed in 2014. The J/ψ yields are measured in a wide transverse momentum (pT) range of 0.15 GeV/c to 12 GeV/c from central to peripheral collisions. They extend the kinematic reach of previous measurements at RHIC with improved precision. In the 0-10% most central collisions, the J/ψ yield is suppressed by a factor of approximately 3 for pT > 5 GeV/c relative to that in p + p collisions scaled by the number of binary nucleon-nucleon collisions. The J/ψ nuclear modification factor displays little dependence on pT in all centrality bins. Model calculations can qualitatively describe the data, providing further evidence for the color-screening effect experienced by J/ψ mesons in the QGP.
Non-standard errors
(2021)
In statistics, samples are drawn from a population in a data-generating process (DGP). Standard errors measure the uncertainty in sample estimates of population parameters. In science, evidence is generated to test hypotheses in an evidence-generating process (EGP). We claim that EGP variation across researchers adds uncertainty: non-standard errors. To study them, we let 164 teams test six hypotheses on the same sample. We find that non-standard errors are sizeable, on par with standard errors. Their size (i) co-varies only weakly with team merits, reproducibility, or peer rating, (ii) declines significantly after peer-feedback, and (iii) is underestimated by participants.
Six species of the spider genus Spinirta Jin & Zhang, 2020 from southern China (Araneae: Corinnidae)
(2024)
In the current study, six species of the genus Spinirta from southern China are recognized, four new species are described: S. hongyui Wang, Lu & Z.S. Zhang sp. nov. (♂♀), S. liuae Wang, Lu & Z.S. Zhang sp. nov. (♂♀), S. simianshan Wang, Lu & Z.S. Zhang sp. nov. (♂♀) and S. yintiaoling Wang, Lu & Z.S. Zhang sp. nov. (♂). Females of S. aviforma Jin & Zhang, 2020 (♂♀) and S. quadrata Jin & Zhang, 2020 (♂♀) are described for the first time. Photos of the body and copulatory organs, as well as the locality map are provided.
Simple Summary
The interaction between tumors and immune cells influences tumor fate, i.e., regression, growth, or even metastases. The evaluation of tumor infiltrating lymphocytes (TILs) in human breast cancer has prognostic value. Pet rabbits develop spontaneous mammary carcinomas and have an immune system that is comparable with that of humans, so that they have the potential to provide an animal model for human breast cancer. To further substantiate this similarity, this study examined TILs in 107 pet rabbit mammary carcinomas according to criteria established for human breast cancer. For TIL evaluation routinely stained microscopic sections were examined by light microscopy. Relevant histological and immunohistochemical tumor characteristics were obtained from a data base. Results showed that increased presence of stromal TILs was statistically associated with histological tumor features indicative of a less aggressive biological behavior, i.e., reduced tumor cell proliferation and a lower histological grade. The expression by tumor cells of calponin, a presumed tumor suppressor protein, was also associated with their reduced proliferation and a higher percentage of stromal TILs. Data suggest that higher percentages of stromal TILs may have the potential to serve as favorable prognostic indicator in rabbit mammary carcinomas and support the value of pet rabbits for comparative research.
Abstract
Tumor infiltrating lymphocytes (TILs) serve as prognostic biomarker in human breast cancer. Rabbits have the potential to act as animal model for human breast cancer, and close similarities exist between the rabbit and human immune system. The aim of this study is to characterize TILs in pet rabbit mammary carcinomas and to statistically correlate results with histological and immunohistochemical tumor characteristics. Microscopic evaluation of TILs was performed in hematoxylin and eosin stained sections of 107 rabbit mammary carcinomas according to international guidelines for human breast cancer. Data on histological features of malignancy, estrogen and progesterone receptor status and calponin expression were obtained from the data base. This study revealed a statistical association between stromal TILs in the central tumor (CT) and infiltrative margin. Higher maximal percentages of stromal TILs at the CT were statistically correlated with decreased mitotic count and lower tumor grade. An increased number of calponin positive tumor cells was statistically associated with a lower mitotic count and a higher percentage of stromal TILs. Results suggest that higher percentages of stromal TILs are useful biomarkers that may point toward a favorable prognosis in rabbit mammary carcinomas and support the concept of the use of rabbits for translational research
A century and a half since the time of Hewitson, we are experiencing a renaissance in species discovery fueled by whole genome sequencing. A large-scale genomic analysis of Hesperiidae Latreille, 1809 (Lepidoptera), including primary type specimens, reveals a deluge of species new to science. One hundred of them (one in a new genus) are described here from the New World (type localities are given in parenthesis): Drephalys (Drephalys) diovalis Grishin, new species (Ecuador: Napo), Euriphellus panador Grishin, new species (Ecuador: Esmeraldas), Euriphellus panamicus Grishin, new species (Panama: Panama), Cecropterus (Thorybes) viridissimus Grishin, new species (Ecuador: Zamora-Chinchipe), Cecropterus (Murgaria) dariensis Grishin, new species (Panama: Darien), Urbanus (Urbanus) mericuti Grishin, new species (Ecuador: Napo), Telegonus (Telegonus) pastus Grishin, new species (Panama: Panama), Autochton (Autochton) dora Grishin, new species (Ecuador: Pastaza), Astraptes centralis Grishin, new species (Panama: Colón), Aguna claxonica Grishin, new species (Ecuador: Napo), Aguna esmeralda Grishin, new species (Ecuador: Esmeraldas), Aguna lata Grishin, new species (Guyana), Ridens angulinea Grishin, new species (Peru: Cuzco), Pythonides lera Grishin, new species (Peru: Cuzco), Pythonides latemarginatus Grishin, new species (Panama: Panama), Gindanes variegatus Grishin, new species (Brazil: Mato Grosso), Milanion (Milanion) virga Grishin, new species (Brazil: Rondônia), Milanion (Milanion) furvus Grishin, new species (Panama: Panama), Milanion (Milanion) laricus Grishin, new species (Ecuador: Napo), Charidia ronda Grishin, new species (Brazil: Rondônia), Pseudodrephalys tinas Grishin, new species (Peru: Loreto), Pseudodrephalys argus Grishin, new species (Suriname: Para), Achlyodes calvus Grishin, new species (Brazil: Santa Catarina), Spioniades artemis Grishin, new species (Panama: Panama), Spioniades artemidoides Grishin, new species (Brazil: Santa Catarina), Myrinia orieca Grishin, new species (Ecuador: Orellana), Myrinia aragua Grishin, new species (Venezuela: Aragua), Myrinia maculosa Grishin, new species (Guatemala), Myrinia manchada Grishin, new species (Guyana), Polyctor (Fenops) lamperus Grishin, new species (Panama: Darien), Nisoniades (Nisoniades) lutum Grishin, new species (Mexico: Guerrero. ), Bolla (Stolla) vena Grishin, new species (Venezuela: Aragua), Staphylus (Vulga) vula Grishin, new species (Mexico: Veracruz), Staphylus (Vulga) vulga Grishin, new species (Panama: Darien), Staphylus (Staphylus) rotundalus Grishin, new species (Ecuador: Napo), Staphylus (Staphylus) yucatanus Grishin, new species (Mexico: Quintana Roo/Yucatan), Heliopetes (Heliopetes) lana Grishin, new species (Guatemala), Canesia ella Grishin, new species (Venezuela: Barinas), Paches (Paches) loxeca Grishin, new species (Ecuador: Morona-Santiago), Clito congruens Grishin, new species (Panama: Colón), Cycloglypha corax Grishin, new species (Brazil: Rio de Janeiro), Festivia peruvia Grishin, new species (Peru: Huánuco), Decinea notata Grishin, new species (Ecuador: Napo), Pompeius fuscus Grishin, new species (Brazil: Minas Gerais), Vernia clara Grishin, new species (Panama: Chiriquí), Oligoria (Oligoria) obtena Grishin, new species (Ecuador: Napo), Thespieus mandal Grishin, new species (Brazil: Rio de Janeiro), Psoralis (Saniba) magnamacus Grishin, new species (Panama: Darien), Alychna ayonis Grishin, new species (Ecuador: Napo), Wahydra banios Grishin, new species (Ecuador: Tungurahua), Wahydra cuzcona Grishin, new species (Peru: Cuzco), Cynea (Cynea) aureofimbra Grishin, new species (Ecuador), Cynea (Nycea) quada Grishin, new species (Ecuador: Napo), Cynea (Quinta) achirae Grishin, new species (Mexico: Tamaulipas), Eutus amazonicus Grishin, new species (Peru: Madre de Dios), Eutus incus Grishin, new species (Peru: Cuzco), Eutus septemaculatus Grishin, new species (Brazil: Mato Grosso), Godmia viridicapita Grishin, new species (Ecuador: Napo), Rhomba pulla Grishin, new species (Peru: Cuzco), Niconiades victoria Grishin, new species (Mexico: Tamaulipas), Lancephallus purpurus Grishin, new genus and new species (Guyana), Mnasicles (Remella) ecua Grishin, new species (Ecuador: Pichincha), Amblyscirtes (Amblyscirtes) aeratus Grishin, new species (Mexico: Oaxaca), Amblyscirtes (Mastor) chrysoplea Grishin, new species (Mexico: Oaxaca), Amblyscirtes (Mastor) chrysomisa Grishin, new species (Mexico: Chiapas), Amblyscirtes (Flor) meridus Grishin, new species (Mexico: Veracruz), Rectava chiriquensis Grishin, new species (Panama: Chiriquí), Cobalopsis adictys Grishin, new species (Panama: Veraguas), Cymaenes melaporphyrus Grishin, new species (Mexico: San Luis Potosí), Lerema (Morys) ecuadorica Grishin, new species (Ecuador: Pichincha), Saturnus obscurior Grishin, new species (Panama: Darien), Cantha zoirodicta Grishin, new species (Peru: Madre de Dios), Cantha meiodicta Grishin, new species (Peru: Madre de Dios), Phlebodes duplex Grishin, new species (Guatemala: Cayuga), Lychnuchus (Enosis) valle Grishin, new species (Colombia: Valle), Eutychide ochoides Grishin, new species (Peru: Cuzco), Dion bora Grishin, new species (Panama: Darien), Dion occida Grishin, new species (Peru: Madre de Dios), Eprius (Eprius) veledinus Grishin, new species (Ecuador: Pichincha), Radiatus panamensis Grishin, new species (Panama: Panama), Pheraeus pulcher Grishin, new species (Peru: Madre de Dios), Callimormus rades Grishin, new species (Panama: Panama), Gubrus lubens Grishin, new species (Ecuador: Loja), Ludens labens Grishin, new species (Panama: Darien), Rigga isa Grishin, new species (Ecuador: Napo), Flaccilla lactea Grishin, new species (Peru: Cuzco), Falga athena Grishin, new species (Panama: Darien), Panoquina jay Grishin, new species (Peru: Loreto), Calpodes salianus Grishin, new species (Peru: Madre de Dios), Calpodes stingo Grishin, new species (Ecuador: Sucumbíos), Aides nobra Grishin, new species (Panama: Colón), Thracides pavo Grishin, new species (Mexico: Tabasco), Talides eluta Grishin, new species (Peru: Cuzco), Talides laeta Grishin, new species (Peru: Cuzco), Neoxeniades angustior Grishin, new species (Brazil: Rio de Janeiro), Damas zea Grishin, new species (Guyana), Tromba xantha Grishin, new species (Mexico: Veracruz), Perichares fura Grishin, new species (Ecuador: Pichincha), Carystoides (Balma) goliath Grishin, new species (Colombia: Valle), and Agathymus galeana Grishin, new species (Mexico: Nuevo Leon). Additionally, we present evidence to support 22 taxa as species (not subspecies or synonyms) and synonymize one genus and four species. Namely, the following taxa are species: Milanion pilta Evans, 1953 (not Milanion pilumnus Mabille and Boullet, 1917), Milanion latior Mabille and Boullet, 1917 (not a synonym of Milanion marciana Godman and Salvin, 1895), Charidia pilea Evans, 1953, and Charidia pocus Evans, 1953 (not Charidia lucaria (Hewitson, 1868)), Paches (Paches) gloriosus Röber, 1925 and Paches (Paches) loxana Evans, 1953 (not Paches (Paches) loxus (Westwood, 1852)), Spioniades anta Evans, 1953 (not Spioniades abbreviata (Mabille, 1888)), Decinea onasima (Hewitson, 1877) and Decinea formosus (Hayward, 1940) (not Decinea dama (Herrich-Schäffer, 1869)), Thespieus guerreronis (Dyar, 1913) (not Thespieus dalman (Latreille, [1824])), Cynea (Nycea) erebina (Möschler, 1879) and Cynea (Nycea) cleochares (Mabille, 1891) (not Cynea (Cynea) diluta (Herrich-Schäffer, 1869)), Amblyscirtes (Mastor) repta Evans, 1955 (not Amblyscirtes (Flor) florus (Godman, 1900)), Saturnus tiberius (Möschler, 1883), Saturnus conspicuus (E. Bell, 1941), Saturnus meton (Mabille, 1891), and Saturnus obscurus (E. Bell, 1941) (not Saturnus reticulata (Plötz, 1883)), Phlebodes sifax Evans, 1955 (not Phlebodes campo (E. Bell, 1947)), Eutychide ochus Godman, 1900 and Eutychide rogersi (Kaye, 1914) (not a subspecies and a synonym, respectively, of Eutychide subcordata (Herrich-Schäffer, 1869)), Falga mirabilis Evans, 1955, Falga jacta Evans, 1955, and Falga ombra Evans, 1955 (not Falga jeconia (A. Butler, 1870)); and the following taxa are junior subjective synonyms: Libra Evans, 1955 (of Phemiades Hübner, [1819]), Papilio clito Fabricius, 1787 of Milanion hemes hemes (Cramer, 1777), Pamphila hycsos Mabille, 1891 of Cynea (Nycea) erebina (Möschler, 1879), Hesperia olympia Plötz, 1882 of Eutychide subcordata (Herrich-Schäffer, 1869), and Hesperia ocrinus Plötz, 1882 of Aides aegita (Hewitson, 1866). Furthermore, we propose new combinations for genus-species: Lychnuchus (Enosis) ponka (Evans, 1955) (not Thoon Godman, 1900), and species-subspecies: Charidia pocus mayo Evans, 1953 (not Charidia lucaria (Hewitson, 1868)), Decinea onasima boliviensis (E. Bell, 1930) (not Decinea dama (Herrich-Schäffer, 1869)), Cynea (Nycea) erebina somba Evans, 1955 (not Pamphila hycsos Mabille, 1891), Saturnus tiberius suffuscus (Hayward, 1940) (not Saturnus reticulata (Plötz, 1883)), and Falga mirabilis odol Evans, 1955 (not Falga jeconia (A. Butler, 1870)). Then, Milanion pilumnus var. hemestinus Mabille and Boullet, 1917 is a junior subjective synonym of Milanion pilumnus pilumnus Mabille and Boullet, 1917, not of Milanion leucaspis (Mabille, 1878). Lectotypes are designated for nine taxa (names in original combinations below): Pellicia bromias Godman and Salvin, 1894 (Mexico: Veracruz, Atoyac), Nisoniades perforata Möschler, 1879 (Colombia), Helias ascalaphus Staudinger, 1876 (central Panama), Pamphila hycsos Mabille, 1891 (Colombia), Amblyscirtes fluonia Godman, 1900 (Mexico: Guerrero, Xocomanatlan), Mastor anubis Godman, 1900 (Mexico: Guerrero, Omiltemi), Eutychide ochus Godman, 1900 (Mexico: Veracruz, Atoyac), Cobalus subcordata Herrich-Schäffer, 1869 (Southeast Brazil), and Thracides xanthura Godman, 1901 (Panama: Chiriquí Province, Bugaba). A neotype is designated for Eudamus briccius Plötz, 1881 (Guyana: Iwokrama Forest).
ZooBank registration. urn:lsid:zoobank.org:pub:ACDF923B-906D-460E-9707-259E0ECDBCA8
Genomic analysis of Pyrginae Burmeister, 1878 (Lepidoptera: Hesperiidae Latreille, 1809) with an emphasis on the tribes Achlyodini Burmeister, 1878 and Carcharodini Verity, 1940 reveals many inconsistencies between the resulting phylogeny and the current classification. These problems are corrected by proposing new taxa, changing the ranks of others, or synonymizing them, and transferring species between genera. As a result, five subtribes, one genus, 20 subgenera, and one species are proposed as new: Cyclosemiina Grishin, new subtribe (type genus Cyclosemia Mabille, 1878), Ilianina Grishin, new subtribe (type genus Iliana E. Bell, 1937), Nisoniadina Grishin, new subtribe (type genus Nisoniades Hübner, [1819]), Burcina Grishin, new subtribe (type genus Burca E. Bell and W. Comstock, 1948), and Pholisorina Grishin, new subtribe (type genus Pholisora Scudder, 1872), all in Carcharodini; Lirra Grishin, new genus (type species Leucochitonea limaea Hewitson, 1868) in Pythonidina Grishin, 2019; Trifa Grishin, new subgenus (type species Tagiades jacobus Plötz, 1884), Tuberna Grishin, new subgenus (type species Pythonides contubernalis Mabille, 1883), Ebona Grishin, new subgenus (type species Quadrus eboneus E. Bell, 1947), Noctis Grishin, new subgenus (type species Achlyodes accedens Mabille, 1895), and Cyrna Grishin, new subgenus (type species Achlyodes cyrna Mabille, 1895) of Quadrus Lindsey, 1925; Liddia Grishin, new subgenus (type species Helias pallida R. Felder, 1869), Minna Grishin, new subgenus (type species Achlyodes minna Evans, 1953), and Thilla Grishin, new subgenus (type species Eurypterus later Mabille, 1891) of Eantis Boisduval, 1836; Torgus Grishin, new subgenus (type species Ouleus gorgus E. Bell, 1937) of Iliana E. Bell, 1937; Fenops Grishin, new subgenus (type species Cabares enops Godman and Salvin, 1894) of Polyctor Evans, 1953; Bezus Grishin, new subgenus (type species Pellicia bessus Möschler, 1877) and Macarius Grishin, new subgenus (type species Pellicia macarius Herrich-Schäffer, 1870) of Nisoniades Hübner, [1819]; Quadralis Grishin, new subgenus (type species Pterygospidea extensa Mabille, 1891) of Gorgopas Godman and Salvin, 1894; Menuda Grishin, new subgenus (type species Nisoniades menuda Weeks, 1902) and Narycus Grishin, new subgenus (type species Pythonides narycus Mabille, 1889) of Perus Grishin, 2019; Bovaria Grishin, new subgenus (type species Achlyodes cyclops Mabille, 1876), Sebia Grishin, new subgenus (type species Nisoniades eusebius Plötz, 1884), and Stolla Grishin, new subgenus (type species Pholisora balsa E. Bell, 1937) of Bolla Mabille, 1903; Vulga Grishin, new subgenus (type species Achlyodes vulgata Möschler, 1879) and Capilla Grishin, new subgenus (type species Helias aurocapilla Staudinger, 1876, currently a junior subjective synonym of Hesperia musculus Burmeister, 1875) of Staphylus Godman and Salvin, 1896; and Quadrus (Zera) vivax Grishin, new species (type locality in Brazil: Rio de Janeiro). The following 10 are subgenera, not genera or synonyms: Ouleus Lindsey, 1925 and Zera Evans, 1953 of Quadrus Lindsey, 1925; Atarnes Godman and Salvin, 1897 and Eburuncus Grishin, 2012 of Milanion Godman and Salvin, 1895; Pachyneuria Mabille, 1888 and Austinus O. Mielke and Casagrande, 2016 of Sophista Plötz, 1879; Hemipteris Mabille, 1889 and Mictris Evans, 1955 of Pellicia Herrich-Schäffer, 1870; and Hesperopsis Dyar, 1905 and Scantilla Godman and Salvin, 1896 of Staphylus Godman and Salvin, 1896. The following 7 are species, not subspecies: Quadrus (Ebona) cristatus (Steinhauser, 1989) (not Quadrus (Ebona) negrus (Nicolay, 1980)), Quadrus (Quadrus) ophia (A. Butler, 1870) (not Quadrus (Quadrus) lugubris (R. Felder, 1869)), Quadrus (Zera) gellius (Mabille, 1903) and Quadrus (Zera) servius (Plötz, 1884) (not Quadrus (Zera) hyacinthinus (Mabille, 1877)), Mimia pazana Evans,1953 (not Mimia phidyle (Godman and Salvin, 1894)), Polyctor (Polyctor) dagua Evans, 1953 (not Polyctor (Polyctor) polyctor (Prittwitz, 1868)), and Staphylus (Vulga) satrap Evans, 1953 (not Staphylus (Vulga) saxos Evans, 1953); and these 8 are species, not synonyms: Quadrus (Zera) menedemus (Godman and Salvin, 1894) (not Quadrus (Zera) tetrastigma (Sepp, [1847])), Pellicia (Pellicia) bilinea Mabille, 1889 (not Pellicia (Pellicia) dimidiata Herrich-Schäffer, 1870), Pellicia (Hemipteris) nema Williams and Bell, 1939 (not Pellicia (Pellicia) theon Plötz, 1882), Bolla (Bovaria) sodalis Schaus, 1913 (not Bolla (Bolla) imbras (Godman and Salvin, 1896)), Bolla (Bovaria) aplica (E. Bell, 1937) (not Bolla (Sebia) eusebius (Plötz, 1884)), Bolla (Sebia) chilpancingo (E. Bell, 1937) (not Bolla (Bolla) subapicatus (Schaus, 1902)), and Bolla (Stolla) madrea (R. Williams and E. Bell, 1940) and Bolla (Stolla) hazelae (Hayward, 1940) (not Bolla (Stolla) zorilla (Plötz, 1886)). The following 2 are junior subjective synonyms: Achlyodes erisichthon Plötz, 1884 of Quadrus (Zera) servius (Plötz, 1884) (not a subspecies of Quadrus (Zera) tetrastigma (Sepp, [1847]) and Staphylus subapicatus Schaus, 1902 of Bolla (Bolla) imbras (Godman and Salvin, 1896). Furthermore, we propose the following additional new genus-species combination: Gindanes homer (Evans, 1953), Gindanes nides (O. Mielke and Casagrande, 2002), Gindanes maraca (O. Mielke and Casagrande, 1992), Gindanes jenmorrisae (Shuey and Ramírez. 2022), Gindanes tullia (Evans, 1953), Gindanes herennius (Geyer, [1838]), Gindanes proxenus (Godman and Salvin, 1895), Gindanes parallelus (Mabille, 1898), Gindanes braga (Evans, 1953), Gindanes hampa (Evans, 1953), Gindanes rosa (Steinhauser, 1989), Gindanes neivai (Hayward, 1940), Gindanes mundo (H. Freeman, 1979), Gindanes eminus (E. Bell, 1934), Quadrus (Trifa) francesius Freeman, 1969, Quadrus (Trifa) ineptus (Draudt, 1922), Quadrus (Trifa) jacobus (Plötz, 1884), Quadrus (Tuberna) lancea (Hewitson, 1868), Quadrus (Ebona) pescada (E. Bell, 1956), Lirra pteras (Godman and Salvin, 1895), and Lirra limaea (Hewitson, 1868) (not Pythonides Hübner, 1819); Quadrus (Cyrna) zora (Evans, 1953) (not Bolla Mabille, 1903); Eantis later (Mabille, 1891) and Eantis haber (Mabille, 1891) (not Aethilla Hewitson, 1868); Iliana (Torgus) gorgus (E. Bell, 1937) and Iliana (Torgus) taurus (Evans, 1953) (not Eantis Boisduval, 1836); Bolla (Stolla) evemerus (Godman and Salvin, 1896), Bolla (Stolla) chlora (Evans, 1953), Bolla (Stolla) astra (R. Williams and E. Bell, 1940), Bolla (Stolla) balsa (E. Bell, 1937), Bolla (Stolla) tridentis (Steinhauser, 1989), Bolla (Stolla) esmeraldus (L. Miller, 1966), Bolla (Stolla) chlorocephala (Latreille, [1824]), and Bolla (Stolla) incanus (E. Bell, 1932) (not Staphylus Godman and Salvin, 1896). Finally, lectotypes are designated for Achlyodes servius Plötz, 1884 (type locality in Brazil: Rio de Janeiro), Pellicia theon Plötz, 1882 (type locality in South America), and Nisoniades eusebius Plötz, 1884 (type locality in Central America). Unless stated otherwise, all subgenera, species, subspecies, and synonyms of mentioned genera and species are transferred with their parent taxa, and others remain as previously classified.
ZooBank registration. http://zoobank.org/B9AFA1A9-8664-4F31-B4D9-ACF7780C7CC6
Genomic sequencing and analysis of worldwide skipper butterfly (Lepidoptera: Hesperiidae) fauna points to imperfections in their current classification. Some tribes, subtribes and genera as they are circumscribed today are not monophyletic. Rationalizing genomic results from the perspective of phenotypic characters suggests two new tribes, two new subtribes and 50 new genera that are named here: Ceratrichiini Grishin, trib. n., Gretnini Grishin, trib. n., Falgina Grishin, subtr. n., Apaustina Grishin, subtr. n., Flattoides Grishin, gen. n., Aurivittia Grishin, gen. n., Viuria Grishin, gen. n., Clytius Grishin, gen. n., Incisus Grishin, gen. n., Perus Grishin, gen. n., Livida Grishin, gen. n., Festivia Grishin, gen. n., Hoodus Grishin, gen. n., Anaxas Grishin, gen. n., Chiothion Grishin, gen. n., Crenda Grishin, gen. n., Santa Grishin, gen. n., Canesia Grishin, gen. n., Bralus Grishin, gen. n., Ladda Grishin, gen. n., Willema Grishin, gen. n., Argemma Grishin, gen. n., Nervia Grishin, gen. n., Dotta Grishin, gen. n., Lissia Grishin, gen. n., Xanthonymus Grishin, gen. n., Cerba Grishin, gen. n., Avestia Grishin, gen. n., Zetka Grishin, gen. n., Turmosa Grishin, gen. n., Mielkeus Grishin, gen. n., Coolus Grishin, gen. n., Daron Grishin, gen. n., Barrolla Grishin, gen. n., Brownus Grishin, gen. n., Tava Grishin, gen. n., Rigga Grishin, gen. n., Haza Grishin, gen. n., Dubia Grishin, gen. n., Pares Grishin, gen. n., Chitta Grishin, gen. n., Artonia Grishin, gen. n., Lurida Grishin, gen. n., Corra Grishin, gen. n., Fidius Grishin, gen. n., Veadda Grishin, gen. n., Tricrista Grishin, gen. n., Viridina Grishin, gen. n., Alychna Grishin, gen. n., Ralis Grishin, gen. n., Testia Grishin, gen. n., Buzella Grishin, gen. n., Vernia Grishin, gen. n., and Lon Grishin, gen. n. In addition, the following taxonomic changes are suggested. Prada Evans is transferred from Hesperiinae to Trapezitinae. Echelatus Godman and Salvin, Systaspes Weeks, and Oenides Mabille are removed from synonymy and are treated as valid genera. The following genera are new junior subjective synonyms: Tosta Evans of Eantis Boisduval; Turmada Evans of Neoxeniades Hayward, Arita Evans of Tigasis Godman, and Alera Mabille of Perichares Scudder. Eantis pallida (R. Felder) (not Achlyodes Hübner), Gindanes kelso (Evans) (not Onenses Godman and Salvin), Isoteinon abjecta (Snellen) (not Astictopterus C. and R. Felder), Neoxeniades ethoda (Hewitson) (not Xeniades Godman), Moeris anna (Mabille) (not Vidius Evans), and Molo pelta Evans (not Lychnuchus Hübner) are new genus-species combinations. The following are species-level taxa: Livida assecla (Mabille) (not a subspecies of Livida grandis (Mabille), formerly Pythonides Hübner) and Alychna zenus (E. Bell) (not a junior subjective synonym of Alychna exclamationis (Mabille), formerly Psoralis Mabille); and Barrolla molla E. Bell (formerly Vacerra Godman) is a junior subjective synonym of Barrolla barroni Evans (formerly Paratrytone Godman). All these changes to taxonomic status of names are propagated to all names currently treated as subspecies (for species), subgenera (for genera) and synonyms of these taxa. Finally, taxa not mentioned in this work are considered to remain at the ranks and in taxonomic groups they have been previously assigned to.
Our expanded efforts in genomic sequencing to cover additional skipper butterfly (Lepidoptera: Hesperiidae) species and populations, including primary type specimens, call for taxonomic changes to restore monophyly and correct misidentifications by moving taxa between genera and proposing new names. Reconciliation between phenotypic characters and genomic trees suggests three new tribes, two new subtribes, 23 new genera, 17 new subgenera and 10 new species that are proposed here: Psolosini Grishin, new tribe (type genus Psolos Staudinger, 1889), Ismini Grishin, new tribe (type genus Isma Distant, 1886), Eetionini Grishin, new tribe (type genus Eetion de Nicéville, 1895), Orphina Grishin, new subtribe (type genus Orphe Godman, 1901), Carystoidina Grishin, new subtribe (type genus Carystoides Godman, 1901), Fulvatis Grishin, new genus (type species Telegonus fulvius Plötz, 1882), Adina Grishin, new genus (type species Nascus adrastor Mabille and Boullet, 1912), Ornilius Grishin, new genus (type species Ornilius rotundus Grishin, new species), Tolius Grishin, new genus (type species Antigonus tolimus Plötz, 1884), Lennia Grishin, new genus (type species Leona lena Evans, 1937), Trida Grishin, new genus (type species Cyclopides barberae Trimen, 1873), Noxys Grishin, new genus (type species Oxynthes viricuculla Hayward, 1951), Gracilata Grishin, new genus (type species Enosis quadrinotata Mabille, 1889), Hermio Grishin, new genus (type species Falga ? hermione Schaus, 1913), Eutus Grishin, new genus (type species Cobalus rastaca Schaus, 1902), Gufa Grishin, new genus (type species Phlebodes gulala Schaus, 1902), Godmia Grishin, new genus (type species Euroto chlorocephala Godman, 1900), Rhomba Grishin, new genus (type species Eutychide gertschi Bell, 1937), Rectava Grishin, new genus (type species Megistias ignarus Bell, 1932), Contrastia Grishin, new genus (type species Hesperia distigma Plötz, 1882), Mit Grishin, new genus (type species Mnasitheus badius Bell, 1930), Picova Grishin, new genus (type species Vorates steinbachi Bell, 1930), Lattus Grishin, new genus (type species Eutocus arabupuana Bell, 1932), Gubrus Grishin, new genus (type species Vehilius lugubris Lindsey, 1925), Koria Grishin, new genus (type species Hesperia kora Hewitson, 1877), Corta Grishin, new genus (type species Eutychide lycortas Godman, 1900), Calvetta Grishin, new genus (type species Hesperia calvina Hewitson, 1866), Oz Grishin, new genus (type species Astictopterus ozias Hewitson, 1878), Praxa Grishin, new subgenus (type species Nascus prax Evans, 1952), Bron Grishin, new subgenus (type species Papilio broteas Cramer, 1780), Turis Grishin, new subgenus (type species Pyrgus 1955, and Synale Mabille, 1904 of Carystus Hübner, [1819]. The following 20 genera are treated as junior subjective synonyms: Leucochitonea Wallengren, 1857 of Abantis Hopffer, 1855; Sapaea Plötz, 1879 and Netrobalane Mabille, 1903 of Caprona Wallengren, 1857; Parasovia Devyatkin, 1996 of Sebastonyma Watson, 1893; Pemara Eliot, 1978 of Oerane Elwes and Edwards, 1897; Ankola Evans, 1937 of Pardaleodes Butler, 1870; Arotis Mabille, 1904 of Mnaseas Godman, 1901; Chalcone Evans, 1955, Hansa Evans, 1955, and Propertius Evans, 1955 of Metrocles Godman, 1900; Jongiana O. Mielke and Casagrande, 2002 of Cobaloides Hayward, 1939; Pamba Evans, 1955 of Psoralis Mabille, 1904; Brownus Grishin, 2019 of Styriodes Schaus, 1913; Mnasilus Godman, 1900 of Papias Godman, 1900; Sucova Evans, 1955 of Mnasitheus Godman, 1900; Pyrrhocalles Mabille, 1904 and Asbolis Mabille, 1904 of Choranthus Scudder, 1872; Miltomiges Mabille, 1903 of Methionopsis Godman, 1901; Sacrator Evans, 1955 of Thracides Hübner, [1819]; and Lychnuchoides Godman, 1901 of Perichares Scudder, 1872. Arunena Swinhoe, 1919 is a junior subjective synonym of Stimula de Nicéville, 1898 (not of Koruthaialos Watson, 1893). The following 27 names are species-level taxa (some in new combinations) reinstated from synonymy: Salantoia gildo (Mabille, 1888) (not Salatis cebrenus (Cramer, 1777)), Bungalotis corentinus (Plötz, 1882) (not Bungalotis midas (Cramer, 1775)), Telegonus cretellus (Herrich-Schäffer, 1869) (not Telegonus cassander (Fabricius, 1793)), Santa palica (Mabille, 1888) (not Chiothion asychis (Stoll, 1780)), Camptopleura cincta Mabille and Boullet, 1917 (not Camptopleura auxo (Möschler, 1879)), Camptopleura orsus (Mabille, 1889) (not Nisoniades mimas (Cramer, 1775)), Metron voranus (Mabille, 1891) and Metron fasciata (Möschler, 1877) (not Metron zimra (Hewitson, 1877)), Limochores catahorma (Dyar, 1916) (not Limochores pupillus (Plötz, 1882)), Pares viridiceps (Mabille, 1889) (not Thoon modius (Mabille, 1889)), Tigasis wellingi (Freeman, 1969) (not Tigasis arita (Schaus, 1902)), Rectava sobrinus (Schaus, 1902) (not Papias phainis Godman, 1900), Nastra subsordida (Mabille, 1891) (not Adlerodea asema (Mabille, 1891), previously in Eutychide Godman, 1900), Lerema pattenii Scudder, 1872 (not Lerema accius (J. E. Smith, 1797)), Lerema (Morys) ancus (Möschler, 1879) (not Cymaenes tripunctus theogenis (Capronnier, 1874)), Cobalopsis zetus (Bell, 1942) (not Cobalopsis nero (Herrich-Schäffer, 1869)), Lerema (Geia) etelka (Schaus, 1902) (not Lerema (Geia) geisa (Möschler, 1879), previously in Morys Godman, 1900), Cymaenes isus (Godman, 1900) (not Cymaenes trebius (Mabille, 1891)), Vehilius labdacus (Godman, 1900) (not Vehilius inca (Scudder, 1872)), Papias amyrna (Mabille, 1891) (not Papias allubita (Butler, 1877), previously in Mnasilus Godman, 1900), Papias integra (Mabille, 1891) (not Papias subcostulata (Herrich-Schäffer, 1870)), Metiscus atheas Godman, 1900 (not Hesperia achelous Plötz, 1882), Dion agassus (Mabille, 1891) (not Dion uza (Hewitson, 1877), previously in Enosis Mabille, 1889), Picova incompta (Hayward, 1942) (not Lerema (Morys) micythus (Godman, 1900), previously in Morys Godman, 1900), Lucida melitaea (Draudt, 1923) (not Lucida lucia (Capronnier, 1874)), Methionopsis modestus Godman, 1901 (not Methionopsis ina (Plötz, 1882)), and Thargella (Volus) volasus (Godman, 1901) (not Eutocus facilis (Plötz, 1884)). The following 57 taxa are elevated from subspecies to species, new status (some in new combinations): Dyscophellus doriscus (Hewitson, 1867) (not Dyscophellus porcius (C. Felder and R. Felder, 1862), Phocides vida (A. Butler, 1872) (not Phocides urania (Westwood, 1852)), Tagiades (Daimio) ceylonica Evans, 1932 (not Tagiades litigiosa Möschler, 1878), Tagiades (Daimio) tubulus Fruhstorfer, 1910 (not Tagiades sambavana Elwes and Edwards, 1897), Tagiades (Daimio) kina Evans, 1934, Tagiades (Daimio) sheba Evans, 1934, Tagiades (Daimio) martinus Plötz, 1884, Tagiades (Daimio) sem Mabille, 1883, and Tagiades (Daimio) neira Plötz, 1885 (not Tagiades trebellius (Hopffer, 1874)), Tagiades (Daimio) korela Mabille, 1891 and Tagiades (Daimio) presbyter Butler, 1882 (not Tagiades nestus (C. Felder, 1860)), Tagiades obscurus Mabille, 1876, Tagiades ravi (Moore, [1866]), Tagiades atticus (Fabricius, 1793), Tagiades titus Plötz, 1884, Tagiades janetta Butler, 1870, Tagiades inconspicua Rothschild, 1915, and Tagiades hovia Swinhoe, 1904 (not Tagiades japetus (Stoll, [1781])), Tagiades silvia Evans, 1934 and Tagiades elegans Mabille, 1877 (not Tagiades gana (Moore, [1866])), Tapena bornea Evans, 1941 and Tapena minuscula Elwes and Edwards, 1897 (not Tapena thwaitesi Moore, [1881]), Darpa dealbata (Distant, 1886) (not Darpa pteria (Hewitson, 1868)), Perus manx (Evans, 1953) (not Perus minor (Schaus, 1902)), Canesia pallida (Röber, 1925) (not Carrhenes canescens (R. Felder, 1869)), Carrhenes conia Evans, 1953 (not Carrhenes fuscescens (Mabille, 1891)), Anisochoria extincta Hayward, 1933 and Anisochoria polysticta Mabille, 1876 (not Anisochoria pedaliodina (Butler, 1870)), Anisochoria verda Evans, 1953 (not Anisochoria minorella Mabille, 1898), Bralus alco (Evans, 1953) (not Bralus albida (Mabille, 1888)), Ephyriades jamaicensis (Möschler, 1879) (not Ephyriades brunnea (Herrich-Schäffer, 1865)), Koruthaialos (Stimula) frena Evans, 1949 (not Koruthaialos focula (Plötz, 1882)), Euphyes kiowah (Reakirt, 1866) (not Euphyes vestris (Boisduval, 1852)), Mnaseas inca Bell, 1930 (not Mnaseas bicolor (Mabille, 1889)), Metron hypochlora (Draudt, 1923) (not Metrocles schrottkyi (Giacomelli, 1911), previously in Metron Godman, 1900), Decinea huasteca (H. Freeman, 1969), Decinea denta Evans, 1955, and Decinea antus (Mabille, 1895) (not Decinea decinea (Hewitson, 1876)), Xeniades pteras Godman, 1900 (not Xeniades chalestra (Hewitson, 1866)), Xeniades difficilis Draudt, 1923 (not Xeniades orchamus (Cramer, 1777)), Xeniades hermoda (Hewitson, 1870) (not Tisias quadrata (HerrichSchäffer, 1869)), Hermio vina (Evans, 1955) (not Hermio hermione (Schaus, 1913), previously in Lento Evans, 1955), Cymaenes loxa Evans, 1955, (not Cymaenes laureolus (Schaus, 1913)), Niconiades peri (Evans, 1955) (not Rhinthon bajula (Schaus, 1902), previously in Neoxeniades Hayward, 1938), Gallio danius (Bell, 1941) (not Vehilius seriatus (Mabille, 1891)), Gallio massarus (E. Bell, 1940) (not Gallio garima (Schaus, 1902) previously in Tigasis Godman, 1900), Cymaenes edata (Plötz, 1882), Cymaenes miqua (Dyar, 1913) and Cymaenes aequatoria (Hayward, 1940) (not Cymaenes odilia (Burmeister, 1878)), Lychnuchus (Enosis) demon (Evans, 1955) (not Lychnuchus (Enosis) immaculata (Hewitson, 1868), previously in Enosis Mabille, 1889), Naevolus naevus Evans, 1955 (not Naevolus orius (Mabille, 1883)), Lucida scopas (Mabille, 1891), Lucida oebasus (Godman, 1900), and Lucida leopardus (Weeks, 1901) (not Lucida lucia (Capronnier, 1874)), Corticea schwarzi (E. Bell, 1941) and Corticea sylva (Hayward, 1942) (not Corticea mendica (Mabille, 1898)), and Choranthus orientis (Skinner, 1920) (not Choranthus antiqua (Herrich-Schäffer, 1863), previously in Pyrrhocalles Mabille, 1904). Borbo impar bipunctata (Elwes and J. Edwards, 1897) is a valid subspecies, not a synonym of Borbo impar tetragraphus (Mabille, 1891), here placed in synonymy with Lotongus calathus (Hewitson, 1876), new synonym. We confirm the species status of Telegonus cassius (Evans, 1952) and Lerema (Morys) valda Evans, 1955. Euphyes chamuli Freeman, 1969 is placed as a subspecies of Euphyes kiowah (Reakirt, 1866), new status. The following 41 taxa are junior subjective synonyms, either newly proposed or transferred from synonymy with other species or subspecies: Telegonus mutius Plötz, 1882 of Euriphellus phraxanor (Hewitson, 1876), Telegonus erythras Mabille, 1888 of Dyscophellus damias (Plötz, 1882), Aethilla jaira Butler, 1870 of Telegonus cretellus (Herrich-Schäffer, 1869), Paches era Evans, 1953 of Santa palica (Mabille, 1888), Antigonus alburnea Plötz, 1884 of Tolius tolimus robigus (Plötz, 1884) (not of Echelatus sempiternus simplicior (Möschler, 1877)), Echelatus depenicillus Strand, 1921 of E. sempiternus simplicior (not of T. tolimus robigus), Antigonus aura Plötz, 1884 of Theagenes dichrous (Mabille, 1878) (not of Helias phalaenoides palpalis (Latreille, [1824])), Achlyodes impressus Mabille, 1889 of Camptopleura orsus (Mabille, 1889), Augiades tania Schaus, 1902 of Metron voranus (Mabille, 1891), Pamphila verdanta Weeks, 1906 of Metron fasciata (Möschler, 1877), Niconiades viridis vista Evans, 1955 of Niconiades derisor (Mabille, 1891), Pamphila binaria Mabille, 1891 of Conga chydaea (A. Butler, 1877) (not of Cynea cynea (Hewitson, 1876)), Psoralis concolor Nicolay, 1980 of Ralis immaculatus (Hayward, 1940), Hesperia dido Plötz, 1882 of Cynea (Quinta) cannae (Herrich-Schäffer, 1869) (not of Lerema lochius (Plötz, 1882)), Proteides osembo Möschler, 1883 of Cynea (Cynea) diluta (Herrich-Schäffer, 1869) (not of Cynea (Quinta) cannae (Herrich-Schäffer, 1869)), Cobalopsis brema E. Bell, 1959 of Eutus rastaca (Schaus, 1902), Psoralis panamensis Anderson and Nakamura, 2019 of Rhomba gertschi (Bell, 1937), Cobalus asella Herrich-Schäffer, 1869 of Amblyscirtes alternata (Grote and Robinson, 1867) (not of Amblyscirtes vialis (W. H. Edwards, 1862)), Papias trimacula Nicolay, 1973 of Nastra subsordida (Mabille, 1891), Pamphila bipunctata Mabille, 1889 and Sarega staurus Mabille, 1904 of Lerema pattenii Scudder, 1872 (not of Cymaenes lumina (Herrich-Schäffer, 1869), previously in Lerema Scudder, 1872), Hesperia aethra Plötz, 1886 of Lerema lineosa (Herrich-Schäffer, 1865) (not of Lerema (Morys) compta Butler, 1877), Megistias miaba Schaus, 1902 of Cobalopsis valerius (Möschler, 1879), Phanis sylvia Kaye, 1914 of Lerema etelka (Schaus, 1902) (not of Lerema (Geia) geisa (Möschler, 1879), previously in Morys Godman, 1900), Carystus odilia Burmeister, 1878, Pamphila trebius Mabille, 1891 and Megistias corescene Schaus, 1902 of Cymaenes lumina (Herrich-Schäffer, 1869), Hesperia phocylides Plötz, 1882 of Cymaenes edata (Plötz, 1882) (not of Lerema accius (J. E. Smith, 1797)), Pamphila xenos Mabille, 1898 of Vehilius inca (Scudder, 1872), Mnasilus guianae Lindsey, 1925 of Papias amyrna (Mabille, 1891), Pamphila nubila Mabille, 1891 of Papias integra (Mabille, 1891) (not of Cynea corisana (Plötz, 1882)), Enosis matheri H. Freeman, 1969 of Metiscus atheas Godman, 1900 (previously in Enosis Mabille, 1889), Hesperia infuscata Plötz, 1882 of Mnaseas derasa derasa (Herrich-Schäffer, 1870) (previously Arotis Mabille, 1904), (not of Papias subcostulata (Herrich-Schäffer, 1870)), Pamphila astur Mabille, 1891 of Metiscus angularis (Möschler, 1877) (not of Cymaenes tripunctus theogenis (Capronnier, 1874)), Anthoptus macalpinei H. Freeman, 1969 of Anthoptus inculta (Dyar, 1918), Methionopsis typhon Godman, 1901 of Methionopsis ina (Plötz, 1882), Methionopsis dolor Evans, 1955 of Thargella volasus (Godman, 1901), Hesperia cinica Plötz, 1882 of Dubiella dubius (Stoll, 1781), Cobalus disjuncta Herrich-Schäffer, 1869 of Dubiella dubius (Stoll, 1781) (not of Vettius lafrenaye (Latreille, [1824])), and Saliana vixen Evans, 1955 of Neoxeniades parna (Evans, 1955). The following are new and revised genusspecies combinations: Euriphellus cebrenus (Cramer, 1777) (not Salatis Evans, 1952), Gorgopas extensa (Mabille, 1891) (not Polyctor Evans, 1953), Clytius shola (Evans, 1953) (not Staphylus Godman and Salvin, 1896), Perus narycus (Mabille, 1889) (not Ouleus Lindsey, 1925), Perus parvus (Steinhauser and Austin, 1993) (not Staphylus Godman and Salvin, 1896), Pholisora litus (Dyar, 1912) (not Bolla Mabille, 1903), Carrhenes decens (A. Butler, 1874) (not Antigonus Hübner, [1819]), Santa palica (Mabille, 1888) (not Chiothion Grishin, 2019), Bralus nadia (Nicolay, 1980) (not Anisochoria Mabille, 1876), Acerbas sarala (de Nicéville, 1889) (not Lotongus Distant, 1886), Caenides sophia (Evans, 1937) (not Hypoleucis Mabille, 1891), Hypoleucis dacena (Hewitson, 1876) (not Caenides Holland, 1896), Dotta tura (Evans, 1951) (not Astictopterus C. Felder and R. Felder, 1860), Nervia wallengrenii (Trimen, 1883) (not Kedestes Watson, 1893), Testia mammaea (Hewitson, 1876) (not Decinea Evans, 1955), Oxynthes trinka (Evans, 1955) (not Orthos Evans, 1955), Metrocles argentea (Weeks, 1901) (not Paratrytone Godman, 1900), Metrocles scitula (Hayward, 1951) (not Mucia Godman, 1900), Metrocles schrottkyi (Giacomelli, 1911) (not Metron Godman, 1900), Niconiades derisor (Mabille, 1891) (not Decinea Evans, 1955), Paratrytone samenta (Dyar, 1914) (not Ochlodes Scudder, 1872), Oligoria (Cobaloides) locutia (Hewitson, 1876) (not Quinta Evans, 1955), Psoralis (Saniba) laska (Evans, 1955) (not Vidius Evans, 1955), Psoralis (Saniba) arva (Evans, 1955) and Psoralis (Saniba) umbrata (Erschoff, 1876) (not Vettius Godman, 1901), Psoralis (Saniba) calcarea (Schaus, 1902) and Psoralis (Saniba) visendus (E. Bell, 1942) (not Molo Godman, 1900), Alychna gota (Evans, 1955) (not Psoralis Mabille, 1904), Adlerodea asema (Mabille, 1891) and Adlerodea subpunctata (Hayward, 1940) (not Eutychide Godman, 1900), Ralis immaculatus (Hayward, 1940) (not Mucia Godman, 1900), Rhinthon braesia (Hewitson, 1867) and Rhinthon bajula (Schaus, 1902) (not Neoxeniades Hayward, 1938), Cymaenes lochius Plötz, 1882 (not Lerema Scudder, 1872), Paracarystus ranka (Evans, 1955) (not Thoon Godman, 1900), Tricrista aethus (Hayward, 1951), Tricrista canta (Evans, 1955), Tricrista slopa (Evans, 1955), Tricrista circellata (Plötz, 1882), and Tricrista taxes (Godman, 1900) (not Thoon Godman, 1900), Gallio madius (E. Bell, 1941) and Gallio seriatus (Mabille, 1891) (not Vehilius Godman, 1900), Gallio garima (Schaus, 1902) (not Tigasis Godman, 1900), Tigasis corope (HerrichSchäffer, 1869) (not Cynea Evans, 1955), Tigasis perloides (Plötz, 1882) (not Cymaenes Scudder, 1872), Amblyscirtes (Flor) florus (Godman, 1900) (not Repens Evans, 1955), Vidius fraus (Godman, 1900) (not Cymaenes Scudder, 1872), Nastra celeus (Mabille, 1891) (not Vehilius Godman, 1900), Nastra nappa (Evans, 1955) (not Vidius Evans, 1955), Vehilius warreni (Weeks, 1901) and Vehilius limae (Lindsey, 1925) (not Cymaenes Scudder, 1872), Cymaenes lumina (Herrich-Schäffer, 1869) (not Lerema Scudder, 1872), Cobalopsis valerius (Möschler, 1879) (not Cobalopsis Godman, 1900), Cobalopsis dictys (Godman, 1900) (not Papias Godman, 1900), Lerema (Morys) venias (Bell, 1942) (not Cobalopsis Godman, 1900), Papias latonia (Schaus, 1913) (not Cobalopsis Godman, 1900), Dion iccius (Evans, 1955) and Dion uza (Hewitson, 1877) (not Enosis Mabille, 1889), Vistigma (Vistigma) opus (Steinhauser, 2008) (not Thoon Godman, 1900), Saturnus fartuga (Schaus, 1902) (not Parphorus Godman, 1900), Phlebodes fuldai (E. Bell, 1930) (not Vettius Godman, 1901), Mnasitheus padus (Evans, 1955) (not Moeris Godman, 1900), Naevolus brunnescens (Hayward, 1939) (not Psoralis Mabille, 1904), Lamponia ploetzii (Capronnier, 1874) (not Vettius Godman, 1901), Mnestheus silvaticus Hayward, 1940 (not Ludens Evans, 1955), Rigga spangla (Evans, 1955) (not Sodalia Evans, 1955), Corticea vicinus (Plötz, 1884) (not Lento Evans, 1955), Mnasalcas thymoetes (Hayward, 1942) (not Mnasicles Godman, 1901), Mnasalcas boyaca (Nicolay, 1973) (not Pamba Evans, 1955), Vertica brasta (Evans, 1955) (not Lychnuchus Hübner, [1831]), Carystina discors Plötz, 1882 (not Cobalus Hübner, [1819]), Zetka irena (Evans, 1955) (not Neoxeniades Hayward, 1938), and Neoxeniades parna (Evans, 1955) (not Niconiades Hübner, [1821]). The following are new or revised species-subspecies combinations: Tagiades neira moti Evans, 1934, Tagiades neira canonicus Fruhstorfer, 1910, Tagiades sheba vella Evans, 1934, Tagiades sheba lola Evans, 1945, Tagiades korela biakana Evans, 1934, Tagiades korela mefora Evans, 1934, Tagiades korela suffusus Rothschild, 1915, Tagiades korela brunta Evans, 1949, Tagiades ravi ravina Fruhstorfer, 1910, Tagiades atticus carnica Evans, 1934, Tagiades atticus nankowra Evans, 1934, Tagiades atticus helferi C. Felder, 1862, Tagiades atticus balana Fruhstorfer, 1910, Tagiades inconspicua mathias Evans, 1934, Tagiades hovia kazana Evans, 1934, Tagiades elegans fuscata de Jong and Treadaway, 2007, Tagiades elegans semperi Fruhstorfer, 1910, Metron hypochlora tomba Evans, 1955, Decinea denta pruda Evans, 1955, and Choranthus orientis eleutherae (Bates, 1934) (previously in Pyrrhocalles Mabille, 1904). In addition to the abovementioned changes, the following new combinations involve newly proposed genus group names: Fulvatis fulvius (Plötz, 1882) and Fulvatis scyrus (E. Bell, 1934) (not Salatis Evans, 1952); Adina adrastor (Mabille and Boullet, 1912) (not Bungalotis Watson, 1893); Nascus (Praxa) prax Evans, 1952, Nascus (Bron) broteas (Cramer, 1780), and Nascus (Bron) solon (Plötz, 1882) (not Pseudonascus Austin, 2008); Chirgus (Turis) veturius (Plötz, 1884); Paches (Tiges) liborius (Plötz, 1884), and Paches (Tiges) mutilatus (Hopffer, 1874) (not Antigonus Hübner, [1819]); Paches (Tiges) exosa (A. Butler, 1877); Tolius tolimus (Plötz, 1884) and Tolius luctuosus (Godman & Salvin, 1894) (not Echelatus Godman and Salvin, 1894); Ancistroides (Ocrypta) caerulea (Evans, 1928), Ancistroides (Ocrypta) renardi (Oberthür, 1878), Ancistroides (Ocrypta) waigensis (Plötz, 1882), Ancistroides (Ocrypta) aluensis (Swinhoe, 1907), Ancistroides (Ocrypta) flavipes (Janson, 1886), and Ancistroides (Ocrypta) maria (Evans, 1949) (not Notocrypta de Nicéville, 1889); Lennia lena (Evans, 1937), Lennia binoevatus (Mabille, 1891), Lennia maracanda (Hewitson, 1876), and Lennia lota (Evans, 1937) (not Leona Evans, 1937); Trida barberae (Trimen, 1873) and Trida sarahae (Henning and Henning, 1998) (not Kedestes Watson, 1893); Noxys viricuculla (Hayward, 1951) (not Oxynthes Godman, 1900); Xeniades (Tixe) quadrata (Herrich-Schäffer, 1869), Xeniades (Tixe) rinda (Evans, 1955), Xeniades (Tixe) putumayo (Constantino and Salazar, 2013) (not Tisias Godman, 1901); Gracilata quadrinotata (Mabille, 1889) (not Styriodes Schaus, 1913); Hermio hermione (Schaus, 1913) (not Lento Evans, 1955); Cynea (Nycea) hycsos (Mabille, 1891), Cynea (Nycea) corisana (Plötz, 1882), Cynea (Nycea) popla Evans, 1955, Cynea (Nycea) iquita (E. Bell, 1941), Cynea (Nycea) robba Evans, 1955, Cynea (Nycea) melius (Geyer, 1832), and Cynea (Nycea) irma (Möschler, 1879); Eutus rastaca (Schaus, 1902) (not Eutychide Godman, 1900); Eutus yesta (Evans, 1955) (not Thoon Godman, 1900); Eutus mubevensis (E. Bell, 1932) (not Tigasis Godman, 1900); Gufa gulala (Schaus, 1902) (not Mucia Godman, 1900); Gufa fusca (Hayward, 1940) (not Tigasis Godman, 1900); Godmia chlorocephala (Godman, 1900) (not Onophas Godman, 1900); Rhomba gertschi (E. Bell, 1937) (not Justinia Evans, 1955); Mnasicles (Nausia) nausiphanes (Schaus, 1913) (not Tigasis Godman, 1900); Amblyscirtes (Flor) florus (Godman, 1900) (not Repens Evans, 1955); Rectava ignarus (E. Bell, 1932) (not Papias Godman, 1900); Rectava vorgia (Schaus, 1902) (not Cobalopsis Godman, 1900); Rectava nostra (Evans, 1955) (not not Vidius Evans, 1955); Lerema (Geia) geisa (Möschler, 1879) and Lerema (Geia) lyde (Godman, 1900) (not Morys Godman, 1900); Contrastia distigma (Plötz, 1882) (not Cymaenes Scudder, 1872); Mit (Mit) badius (E. Bell, 1930) (not Styriodes Schaus, 1913); Mit (Mit) gemignanii (Hayward, 1940), (not Mnasitheus Godman, 1900); Mit (Rotundia) schausi (Mielke and Casagrande, 2002), (not Enosis Mabille, 1889); Picova steinbachi (E. Bell, 1930) (not Saturnus Evans, 1955); Lattus arabupuana (E. Bell, 1932) (not Eutocus Godman, 1901); Gubrus lugubris (Lindsey, 1925) (not Vehilius Godman, 1900); Thargella (Pseudopapias) tristissimus (Schaus, 1902) (not Papias Godman, 1900); Koria kora (Hewitson, 1877) (not Justinia Evans, 1955); Justinia (Septia) septa Evans, 1955; Corta lycortas (Godman, 1900) (not Orthos Evans, 1955); Vertica (Brasta) brasta (Evans, 1955) (not Lychnuchus Hübner, [1831]); Calvetta calvina (Hewitson, 1866) (not Cobalus Hübner, [1819]); Neoxeniades (Bina) gabina (Godman, 1900) (not Orthos Evans, 1955); Oz ozias (Hewitson, 1878) and Oz sebastiani Salazar and Constantino, 2013 (not Lychnuchoides Godman, 1901); and Carystoides (Balma) balza Evans, 1955 and Carystoides (Balma) maroma (Möschler, 1877). Finally, unless stated otherwise, all subgenera, species, subspecies and synonyms of mentioned genera and species are transferred together with their parent taxa, and taxa not mentioned in this work remain as previously classified.
New taxa in Hesperiidae (Lepidoptera: Papilionoidea) are traditionally proposed after inspection of male genitalia, which largely form the basis for Hesperiidae taxonomy. However, with genomic DNA sequencing, even a single female specimen can be placed in a phylogenetic context of existing classification and taxonomically assigned with confidence. Genomic sequencing of an unusually patterned Hesperiidae female from San Martin, Peru, characterized by pearly spots outlining an inverted heart pattern on the rust-colored ventral hindwing, reveals that it represents an undescribed genus and species named here as Gemmia buechei Brockmann and Grishin, new genus and new species.
ZooBank registration. https://zoobank.org/2FA538FA-7D65-4097-9BBA-71CD1B2795E5
Analyses of whole genomic shotgun datasets, COI barcodes, morphology, and historical literature suggest that the following 13 butterfly species from the family Hesperiidae (Lepidoptera: Papilionoidea) in Texas, USA are distinct from their closest named relatives and therefore are described as new (type localities are given in parenthesis): Spicauda atelis Grishin, new species (Hidalgo Co., Mission), Urbanus (Urbanus) rickardi Grishin, new species (Hidalgo Co., nr. Madero), Urbanus (Urbanus) oplerorum Grishin, new species (Hidalgo Co., Mission/Madero), Telegonus tsongae Grishin, new species (Starr Co., Roma), Autochton caballo Grishin, new species (Hidalgo Co., 6 mi W of Hidalgo), Epargyreus fractigutta Grishin, new species (Hidalgo Co., McAllen), Aguna mcguirei Grishin, new species (Cameron Co., Brownsville), Polygonus pardus Grishin, new species (Hidalgo Co., McAllen), Arteurotia artistella Grishin, new species (Hidalgo Co., Mission), Heliopetes elonmuski Grishin, new species (Cameron Co., Boca Chica), Hesperia balcones Grishin, new species (Travis Co., Volente), Troyus fabulosus Grishin, new species (Hidalgo Co., Peñitas), and Lerema ochrius Grishin, new species (Hidalgo Co., nr. Relampago). Most of these species are known in the US almost exclusively from the Lower Rio Grande Valley in Texas. Nine of the holotypes were collected in 1971-1975, a banner period for butterfly species newly recorded from the Rio Grande Valley of Texas; five of them collected by William W. McGuire, and one by Nadine M. McGuire. At the time, these new species have been recorded under the names of their close relatives. A Neotype is designated for Papilio fulminator Sepp, [1841] (Suriname). Lectotypes are designated for Goniurus teleus Hübner, 1821 (unknown, likely in South America), Goniloba azul Reakirt, [1867] (Mexico: Veracruz) and Eudamus misitra Plötz, 1881 (Mexico). Several taxonomic changes are proposed. The following taxa are species (not subspecies): Spicauda zalanthus (Plötz, 1880), reinstated status (not Spicauda teleus (Hübner, 1821)), Telegonus fulminator (Sepp, [1841]), reinstated status (not Telegonus fulgerator (Walch, 1775), Telegonus misitra (Plötz, 1881), reinstated status (not Telegonus azul (Reakirt, [1867])), Autochton reducta (Mabille and Boullet, 1919), new status (not Autochton potrillo (Lucas, 1857)), Epargyreus gaumeri Godman and Salvin, 1893, reinstated status (not Epargyreus clavicornis (Herrich-Schäffer, 1869)), and Polygonus punctus E. Bell and W. Comstock, 1948, new status (not Polygonus savigny (Latreille, [1824])). Urbanus ehakernae Burns, 2014 and Epargyreus socus chota Evans, 1952 are junior subjective synonyms of Urbanus alva Evans, 1952 and Epargyreus clavicornis (Herrich-Schäffer, 1869), respectively, and Epargyreus gaumeri tenda Evans, 1955, new combination is not a subspecies of E. clavicornis.
ZooBank registration. https://zoobank.org/D5462F9E-E08D-46C6-898D-76EE7466DD19