name stringlengths 1 11.3k | aliases listlengths 0 3.27k | kind stringclasses 9
values | role stringclasses 4
values | salience stringclasses 3
values | claims listlengths 0 21 | bibcode stringlengths 19 19 |
|---|---|---|---|---|---|---|
212Po | [
"polonium-212"
] | object | subject | high | [
{
"is_quantitative": false,
"text": "The alpha-decay width of 212Po is calculated using a quartetting wave function approach and agrees fairly well with the measured value."
},
{
"is_quantitative": false,
"text": "The alpha-cluster preformation probability and alpha-decay width of 212Po are micr... | 2016MNRAS.461.4335A |
quartetting wave function approach | [
"quartetting"
] | method | subject | high | [
{
"is_quantitative": false,
"text": "The quartetting wave function approach is improved by implementing four-nucleon correlations to describe alpha preformation in 212Po."
}
] | 2016MNRAS.461.4335A |
208Pb | [
"lead-208"
] | object | used | medium | [
{
"is_quantitative": false,
"text": "The measured density distribution of the 208Pb core is used to calculate the alpha-decay width of 212Po."
}
] | 2016MNRAS.461.4335A |
Ponos | [
"Ponos zoom-in numerical simulations"
] | simulation | subject | high | [
{
"is_quantitative": true,
"text": "The Ponos simulations model dark matter substructures in massive elliptical galaxy halos with virial masses of 1.2 !x 10^{13} M_sun and 6.5 !x 10^{12} M_sun down to z = 0."
},
{
"is_quantitative": true,
"text": "The simulations resolve halos with up to 921,651... | 2016A&A...594A..93C |
dark matter substructures | [
"subhalos"
] | concept | subject | high | [
{
"is_quantitative": true,
"text": "Subhalos with M_sub < 10^9 M_sun contribute between one-fifth and one-third of the total projected mass fraction in massive elliptical halos."
},
{
"is_quantitative": false,
"text": "Baryonic contraction increases the number of massive subhalos in the inner re... | 2016A&A...594A..93C |
baryonic contraction | [] | concept | subject | medium | [
{
"is_quantitative": false,
"text": "Baryonic contraction produces a super-isothermal total density profile and increases the number of massive subhalos in the inner regions of the main host."
}
] | 2016A&A...594A..93C |
gravitational lenses | [] | concept | compared | low | [
{
"is_quantitative": false,
"text": "The host density profiles and projected subhalo mass fractions from the Ponos simulations are broadly consistent with observations of gravitational lenses."
}
] | 2016A&A...594A..93C |
Auger Engineering Radio Array | [
"AERA"
] | facility | subject | high | [
{
"is_quantitative": true,
"text": "AERA consists of more than 150 autonomous radio stations with different spacings, covering an area of about 17 km^2."
},
{
"is_quantitative": true,
"text": "AERA detects radio emission from extensive air showers with energies beyond 10^17 eV in the 30 - 80 MHz... | 2017JCoPh.330..566S |
Pierre Auger Cosmic-Ray Observatory | [
"Auger Observatory"
] | facility | used | medium | [] | 2017JCoPh.330..566S |
Auger surface detector | [] | facility | used | medium | [
{
"is_quantitative": false,
"text": "The Auger surface detector is used to cross-calibrate AERA's radio radiation energy measurements to establish cosmic-ray energy scales."
}
] | 2017JCoPh.330..566S |
radiation energy | [] | concept | subject | high | [
{
"is_quantitative": false,
"text": "The radiation energy emitted by air showers in the form of radio emission is measured and calibrated against the cosmic-ray energy scale."
}
] | 2017JCoPh.330..566S |
lattice field theory methods | [
"lattice methods"
] | method | subject | high | [
{
"is_quantitative": false,
"text": "Lattice field theory methods are increasingly applied to calculate ground-state and thermal properties of strongly interacting non-relativistic few- and many-body systems."
}
] | 2013Icar..223..460S |
hybrid Monte Carlo | [] | method | subject | medium | [
{
"is_quantitative": false,
"text": "Hybrid Monte Carlo techniques have recently crossed over from quantum chromodynamics to condensed matter, atomic, and low-energy nuclear physics."
}
] | 2013Icar..223..460S |
improved effective actions | [] | method | subject | medium | [
{
"is_quantitative": false,
"text": "Improved effective actions have recently been applied to non-relativistic strongly interacting many-body systems."
}
] | 2013Icar..223..460S |
fermions in the limit of unitarity | [] | concept | subject | medium | [
{
"is_quantitative": false,
"text": "Lattice methods are used to determine the ground- and excited-state properties of fermions in the limit of unitarity."
}
] | 2013Icar..223..460S |
intragroup medium | [
"intragroup"
] | concept | subject | high | [
{
"is_quantitative": false,
"text": "The intragroup medium has lower entropy levels and different radial profiles compared to the intracluster medium due to weakly supersonic gas inflow and less effective conversion of kinetic to thermal energy."
}
] | 2016ApJ...830..141L |
intracluster medium | [
"intracluster"
] | concept | subject | high | [
{
"is_quantitative": false,
"text": "The intracluster medium experiences highly supersonic gas inflow across the system boundary, leading to strong accretion shocks and substantial conversion of bulk kinetic into thermal energy."
}
] | 2016ApJ...830..141L |
ESO 3060170 | [] | object | subject | medium | [
{
"is_quantitative": false,
"text": "X-ray observations of the galaxy group ESO 3060170 out to its virial radius show entropy profiles that match theoretical expectations of starved inflow in low-redshift or poor environments."
}
] | 2016ApJ...830..141L |
RXJ1159+5531 | [] | object | subject | medium | [
{
"is_quantitative": false,
"text": "X-ray observations of the galaxy group RXJ1159+5531 out to its virial radius show entropy profiles that match theoretical expectations of starved inflow in low-redshift or poor environments."
}
] | 2016ApJ...830..141L |
iron nanoparticles | [
"metallic iron nanoparticles",
"iron clusters",
"ultrasmall iron clusters"
] | concept | subject | high | [
{
"is_quantitative": true,
"text": "Iron nanoparticles are stable against sublimation in the interstellar radiation field down to a radius of ≃4.5 Å, and potentially smaller."
},
{
"is_quantitative": false,
"text": "Iron nanoparticles can acquire negative charges, particularly in interstellar en... | 2017AdSpR..59..736B |
photoelectric heating | [
"photoelectric heating rate"
] | concept | subject | medium | [
{
"is_quantitative": true,
"text": "The photoelectric heating rate from dust may be increased by up to tens of percent if ≳10% of interstellar iron is in the form of ultrasmall iron clusters."
}
] | 2017AdSpR..59..736B |
interstellar dust | [
"dust"
] | concept | mentioned | low | [] | 2017AdSpR..59..736B |
QSOs | [
"QSO"
] | concept | subject | high | [
{
"is_quantitative": true,
"text": "The host galaxies of nine QSOs at 0.1 < z < 0.2 have black hole masses of 3x10^7 M_sun to 3x10^9 M_sun and far-infrared luminosities of ~ several times 10^11 L_sun."
},
{
"is_quantitative": true,
"text": "The observed L_[OI]63um/L_FIR and L_[CII]/L_FIR ratios ... | 2016A&A...595A..83E |
Herschel Space Observatory | [
"Herschel"
] | facility | used | high | [] | 2016A&A...595A..83E |
[O I] 63 um | [
"[O I] 63 μm"
] | concept | subject | high | [
{
"is_quantitative": true,
"text": "The [O I] 63 um emission is detected in 6 out of 8 observed QSO sources."
}
] | 2016A&A...595A..83E |
[C II] 158 um | [
"[C II] 158 μm",
"[C II]"
] | concept | subject | high | [
{
"is_quantitative": true,
"text": "The [C II] 158 um emission is detected in 8 out of 9 observed QSO sources."
}
] | 2016A&A...595A..83E |
W0752+19 | [] | object | subject | high | [
{
"is_quantitative": true,
"text": "Shows an additional broad velocity component (~720 km s^-1) and exceptionally strong [O I] 63 um emission with L_[OI]63um/L_FIR of 10^-2."
},
{
"is_quantitative": true,
"text": "The gas with broad velocity width in W0752+19 has n_H >= 10^4.3 cm^-3 and G_0 > 10... | 2016A&A...595A..83E |
Sloan Digital Sky Survey | [
"SDSS"
] | survey | used | medium | [] | 2016A&A...595A..83E |
ULIRGs | [
"local ULIRGs",
"local (U)LIRGs"
] | concept | compared | medium | [] | 2016A&A...595A..83E |
ammonia | [
"14NH3",
"15NH3",
"ammonia isotopomers"
] | concept | subject | high | [
{
"is_quantitative": false,
"text": "The hyperfine structure of the rotation-inversion (v2 = 0+, 0-, 1+, 1-) states of 14NH3 and 15NH3 is rationalized in terms of effective hyperfine-structure functions."
},
{
"is_quantitative": false,
"text": "The deperturbed band centers of ammonia can serve a... | 2016AJ....152...83L |
effective hyperfine-structure functions | [
"hfs functions"
] | method | subject | high | [
{
"is_quantitative": false,
"text": "The hfs functions are determined by fitting to available experimental data using Hougen's effective hyperfine-structure Hamiltonian within the framework of the non-rigid inverter theory."
},
{
"is_quantitative": false,
"text": "The fitted hfs functions involv... | 2016AJ....152...83L |
Hougen's effective hyperfine-structure Hamiltonian | [] | method | used | medium | [] | 2016AJ....152...83L |
non-rigid inverter theory | [] | method | used | medium | [] | 2016AJ....152...83L |
proton-to-electron mass ratio | [] | concept | mentioned | low | [] | 2016AJ....152...83L |
atmospheric depth of the shower maximum | [
"X_max",
"X<sub>max</sub>"
] | concept | subject | high | [
{
"is_quantitative": false,
"text": "X_max is strongly correlated with the mass of the primary cosmic ray because it depends on the interaction cross section of the primary with atmospheric constituents."
},
{
"is_quantitative": true,
"text": "X_max can be reconstructed using radio signal amplit... | 2017JCAP...01..027C |
Auger Engineering Radio Array | [
"AERA"
] | facility | used | high | [
{
"is_quantitative": true,
"text": "AERA measures the electric field emitted by secondary particles of extensive air showers in the 30-80 MHz band."
}
] | 2017JCAP...01..027C |
cosmic-ray mass composition | [] | concept | subject | medium | [
{
"is_quantitative": true,
"text": "The statistical determination of the cosmic-ray mass composition is possible through the study of a large number of cosmic rays above 10^17 eV using radio detectors with a duty cycle close to 100%."
}
] | 2017JCAP...01..027C |
scalar-tensor theories of gravity | [
"ST theories",
"ST"
] | concept | subject | high | [
{
"is_quantitative": false,
"text": "The parameter space of scalar-tensor theories of gravity can be constrained by the stability properties of highly compact, massive neutron stars."
},
{
"is_quantitative": false,
"text": "Observations of the most massive neutron stars support a bound on the ST... | 2016PhRvD..94d4062O |
neutron stars | [
"compact stars",
"stars"
] | concept | subject | high | [
{
"is_quantitative": false,
"text": "Highly compact neutron stars in scalar-tensor gravity can become unstable, with the instability driving the stars to collapse in some cases."
}
] | 2016PhRvD..94d4062O |
general relativity | [] | concept | compared | low | [] | 2016PhRvD..94d4062O |
magnetic flux ropes | [
"MFR",
"MFRs"
] | concept | subject | high | [
{
"is_quantitative": false,
"text": "The closed quasi-separatrix layer (QSL) structure surrounding the MFR becomes smaller as a consequence of flare occurrence."
},
{
"is_quantitative": false,
"text": "The twist number of the MFR varies more sensitively than other parameters with the occurrence ... | 2016ApJ...827L..27P |
active region 12017 | [
"AR 12017"
] | object | subject | high | [
{
"is_quantitative": true,
"text": "AR 12017 triggered 12 flares from 2014 March 28-29 due to intermittent eruptions of a filament."
},
{
"is_quantitative": false,
"text": "Flares in AR 12017 during 2014 March 28-29 were mainly triggered by kink instability."
}
] | 2016ApJ...827L..27P |
Helioseismic and Magnetic Imager | [
"HMI"
] | facility | used | medium | [] | 2016ApJ...827L..27P |
Solar Dynamics Observatory | [
"SDO"
] | facility | used | low | [] | 2016ApJ...827L..27P |
nonlinear force-free field model | [
"NLFFF"
] | method | used | medium | [] | 2016ApJ...827L..27P |
kink instability | [] | concept | subject | medium | [
{
"is_quantitative": false,
"text": "Kink instability is found to be the main trigger for the 12 flares observed in AR 12017 from 2014 March 28-29."
}
] | 2016ApJ...827L..27P |
PHENIX experiment | [
"PHENIX"
] | facility | used | high | [
{
"is_quantitative": true,
"text": "The PHENIX experiment measured the cumulants (C_n, n=1,...,4) of net-charge distributions within pseudorapidity |η| < 0.35 in Au+Au collisions at center-of-mass energies of 7.7 to 200 GeV."
}
] | 2016MNRAS.461.4505J |
net-charge multiplicity distributions | [
"net-charge distributions"
] | concept | subject | high | [
{
"is_quantitative": false,
"text": "The ratios of cumulants (C_1/C_2, C_3/C_1) of the net-charge distributions are well described by expectations from negative binomial distributions."
},
{
"is_quantitative": true,
"text": "No nonmonotonic behavior is observed in the ratios of the cumulants of ... | 2016MNRAS.461.4505J |
Relativistic Heavy Ion Collider | [
"RHIC"
] | facility | used | medium | [] | 2016MNRAS.461.4505J |
lattice quantum-chromodynamics | [
"lattice QCD"
] | method | compared | medium | [
{
"is_quantitative": false,
"text": "The measured values of C_1/C_2 and C_3/C_1 can be directly compared to lattice quantum-chromodynamics calculations to extract the chemical freeze-out temperature and baryon chemical potential."
}
] | 2016MNRAS.461.4505J |
thermal-statistical analysis model | [] | method | compared | medium | [
{
"is_quantitative": false,
"text": "The extracted baryon chemical potentials from the net-charge cumulants are in excellent agreement with a thermal-statistical analysis model."
}
] | 2016MNRAS.461.4505J |
1H 0323+342 | [] | object | subject | high | [
{
"is_quantitative": true,
"text": "The Hbeta emission line in 1H 0323+342 has a delayed response of 14.8_{-2.7}^{+3.9} days with respect to the SDSS g' light curve in the rest frame."
},
{
"is_quantitative": true,
"text": "The optical Fe II variations in 1H 0323+342 show a reverberation delay o... | 2016ARep...60..563S |
Lijiang 2.4 m Telescope | [] | facility | used | medium | [
{
"is_quantitative": false,
"text": "Used to monitor 1H 0323+342 for more than two months."
}
] | 2016ARep...60..563S |
SDSS g' | [] | survey | used | low | [] | 2016ARep...60..563S |
Magorrian relation | [] | concept | compared | low | [
{
"is_quantitative": true,
"text": "Predicts a black hole mass for 1H 0323+342 that is one order of magnitude larger than the reverberation mapping mass."
}
] | 2016ARep...60..563S |
compressed sensing | [] | method | subject | high | [
{
"is_quantitative": false,
"text": "Compressed sensing techniques are modified to be compatible with the Gaussian process framework for fast, simultaneous multi-planet radial velocity searches."
},
{
"is_quantitative": false,
"text": "The compressed sensing method produces a periodogram-like ou... | 2017MNRAS.465..997C |
Gaussian process | [] | method | used | high | [
{
"is_quantitative": false,
"text": "Gaussian processes are integrated with compressed sensing techniques to model radial velocity data."
}
] | 2017MNRAS.465..997C |
Lomb-Scargle periodogram | [] | method | compared | medium | [
{
"is_quantitative": false,
"text": "The proposed compressed sensing tool has a similar aspect to the Lomb-Scargle periodogram but exhibits fewer peaks due to aliasing."
}
] | 2017MNRAS.465..997C |
HD 69830 | [] | object | subject | medium | [
{
"is_quantitative": false,
"text": "Analysis of HD 69830 radial velocity data using the compressed sensing method yields results fully compatible with previous analyses."
}
] | 2017MNRAS.465..997C |
HD 10180 | [] | object | subject | medium | [
{
"is_quantitative": false,
"text": "Analysis of HD 10180 radial velocity data using the compressed sensing method yields results fully compatible with previous analyses."
}
] | 2017MNRAS.465..997C |
55 Cnc | [] | object | subject | high | [
{
"is_quantitative": false,
"text": "Analysis of 55 Cnc radial velocity data using the compressed sensing method yields results fully compatible with previous analyses."
},
{
"is_quantitative": false,
"text": "55 Cnc e and f could have been respectively detected and suspected in early measuremen... | 2017MNRAS.465..997C |
GJ 876 | [] | object | subject | high | [
{
"is_quantitative": false,
"text": "Analysis of GJ 876 radial velocity data using the compressed sensing method yields results fully compatible with previous analyses."
},
{
"is_quantitative": false,
"text": "Frequencies due to dynamical interactions in GJ 876 can be resolved using the compress... | 2017MNRAS.465..997C |
Lick Observatory | [] | facility | used | low | [] | 2017MNRAS.465..997C |
Hobby-Eberly Telescope | [] | facility | used | low | [] | 2017MNRAS.465..997C |
Epsilon Eridani | [] | object | subject | high | [
{
"is_quantitative": false,
"text": "Simultaneous ground-based radial velocity and space-based photometric measurements were obtained to explore methods of distinguishing stellar photospheric velocities from Keplerian motion."
}
] | 2016ApJ...830...84K |
Dalmatian | [] | software | subject | medium | [
{
"is_quantitative": false,
"text": "Dalmatian is an MCMC spot modeling code that fits photometric and RV measurements simultaneously."
}
] | 2016ApJ...830...84K |
FF' method | [] | method | subject | medium | [
{
"is_quantitative": false,
"text": "The FF' method uses photometric measurements to predict the stellar activity signal in simultaneous RV measurements."
}
] | 2016ApJ...830...84K |
HH' method | [] | method | subject | high | [
{
"is_quantitative": false,
"text": "The HH' method is a new technique that uses H-alpha measurements as input into the FF' model to predict stellar activity signals."
}
] | 2016ApJ...830...84K |
Microvariability and Oscillations of STars telescope | [
"MOST"
] | facility | used | medium | [
{
"is_quantitative": false,
"text": "MOST photometry of Epsilon Eridani is strongly correlated with simultaneous ground-based H-alpha measurements."
}
] | 2016ApJ...830...84K |
COSMOS J100054.83+023126.2 | [] | object | subject | high | [
{
"is_quantitative": true,
"text": "COSMOS J100054.83+023126.2 is detected in H I 21 cm emission at z = 0.376, representing the highest redshift H I emission detection to date."
},
{
"is_quantitative": true,
"text": "The total H I mass of the galaxy is (2.9 \u0000 1.0) \u0000 10^10 M_sun."
},
... | 2016A&A...594A..74C |
COSMOS H I Large Extragalactic Survey | [
"CHILES"
] | survey | used | high | [
{
"is_quantitative": true,
"text": "CHILES is designed to simultaneously observe H I from z = 0 to z ~ 0.5."
},
{
"is_quantitative": true,
"text": "The first 178 hr of CHILES data were used to detect H I emission in a galaxy at z = 0.376."
}
] | 2016A&A...594A..74C |
Karl G. Jansky Very Large Array | [
"VLA"
] | facility | used | medium | [] | 2016A&A...594A..74C |
Large Millimeter Telescope | [
"LMT"
] | facility | used | medium | [] | 2016A&A...594A..74C |
TorPeDO | [
"dual torsion pendulum sensor"
] | facility | subject | high | [
{
"is_quantitative": false,
"text": "TorPeDO is a dual torsion pendulum sensor designed to measure local gravitational forces to high precision and explore low-frequency gravitational-force noise."
},
{
"is_quantitative": true,
"text": "The sensor features two torsion pendulums with a common sus... | 2016JKAS...49..137H |
Newtonian Noise | [] | concept | mentioned | medium | [] | 2016JKAS...49..137H |
gravitational wave detectors | [] | facility | mentioned | low | [] | 2016JKAS...49..137H |
sunward-propagating Alfvénic fluctuations | [
"SAFs"
] | concept | subject | high | [
{
"is_quantitative": true,
"text": "The percentage of SAFs increases gradually with heliocentric distance, from about 2.7% at 1.0 au to about 8.7% at 5.5 au."
},
{
"is_quantitative": false,
"text": "SAFs can occur in the anti-sunward magnetic sector with a strong positive correlation between mag... | 2016ApJ...831..133H |
anti-sunward-propagating Alfvénic fluctuations | [
"AFs"
] | concept | mentioned | low | [] | 2016ApJ...831..133H |
Voyager 2 | [] | facility | used | high | [
{
"is_quantitative": false,
"text": "Voyager 2 measurements inside 6 au were used to identify and statistically analyze sunward-propagating Alfvénic fluctuations."
}
] | 2016ApJ...831..133H |
Wind | [] | facility | used | high | [
{
"is_quantitative": false,
"text": "Wind spacecraft measurements were used to analyze sunward-propagating Alfvénic fluctuations at 1 au."
}
] | 2016ApJ...831..133H |
FRB 150418 | [] | object | subject | high | [
{
"is_quantitative": false,
"text": "The reported radio counterpart of FRB 150418 is consistent with scintillating radio emission from a compact active galactic nucleus, which would invalidate its association with the FRB."
}
] | 2016ApJ...828...98R |
interstellar scintillation | [
"refractive scintillation"
] | concept | subject | high | [
{
"is_quantitative": false,
"text": "Refractive scintillation in the ionized interstellar medium of the Milky Way can explain the observed 5.5 and 7.5 GHz variability of the putative FRB 150418 counterpart."
}
] | 2016ApJ...828...98R |
active galactic nucleus | [
"AGN"
] | concept | subject | medium | [
{
"is_quantitative": true,
"text": "The putative counterpart of FRB 150418 is consistent with a radio-loud AGN having a brightness temperature T_b >= 10^9 K."
}
] | 2016ApJ...828...98R |
VISTA Variables in Via Lactea | [
"VVV"
] | survey | used | high | [
{
"is_quantitative": false,
"text": "The VVV survey database is used to measure proper motions in the densest regions of the Milky Way bulge and southern plane."
}
] | 2017MNRAS.468.1123S |
Two Micron All Sky Survey | [
"2MASS"
] | survey | used | medium | [
{
"is_quantitative": false,
"text": "The large time baseline between 2MASS and VVV observations is utilized to obtain 2MASS-VVV proper motions."
}
] | 2017MNRAS.468.1123S |
VVV high proper motion stars catalogue | [] | dataset | subject | high | [
{
"is_quantitative": true,
"text": "The catalogue includes 3003 moving stellar sources with Ks <= 13.5 in the VVV survey area."
},
{
"is_quantitative": false,
"text": "The catalogue is in very good agreement with proper motion data supplied in IR catalogues outside the densest zone of the Milky ... | 2017MNRAS.468.1123S |
M-dwarfs | [] | concept | subject | medium | [
{
"is_quantitative": false,
"text": "The majority of the proper motion objects in the VVV high proper motion catalogue are nearby M-dwarfs."
}
] | 2017MNRAS.468.1123S |
common proper motion binary candidates | [] | concept | subject | medium | [
{
"is_quantitative": true,
"text": "57 common proper motion binary candidates are identified, including two new systems within 30 pc of the Sun."
}
] | 2017MNRAS.468.1123S |
GALactic Archeology with Hermes | [
"GALAH"
] | survey | subject | high | [
{
"is_quantitative": true,
"text": "The GALAH survey targets 1 million stars brighter than magnitude V = 14 at a resolution of 28 000 with a goal to measure the abundances of 29 elements."
},
{
"is_quantitative": true,
"text": "GALAH data quality exhibits fibre cross-talk levels of ≲0.5 per cent... | 2017MNRAS.465.4026B |
HERMES | [] | facility | used | medium | [
{
"is_quantitative": true,
"text": "HERMES is a fibre-fed, multi-object spectrograph mounted on the 3.9-m Anglo-Australian Telescope."
}
] | 2017MNRAS.465.4026B |
Anglo-Australian Telescope | [
"AAT"
] | facility | used | low | [] | 2017MNRAS.465.4026B |
IRAF | [] | software | used | medium | [
{
"is_quantitative": false,
"text": "The GALAH reduction pipeline is built using existing IRAF routines to ensure simple maintenance and reliability."
}
] | 2017MNRAS.465.4026B |
GALAH reduction pipeline | [] | software | subject | high | [
{
"is_quantitative": false,
"text": "The pipeline is optimized for speed, accuracy, and consistency to produce fully calibrated spectra for subsequent stellar atmospheric parameter estimation."
}
] | 2017MNRAS.465.4026B |
Higgs boson | [
"H"
] | concept | subject | high | [
{
"is_quantitative": true,
"text": "For a Higgs boson with a mass of 125 GeV, the upper bound on the branching fraction of H to invisible particles is set to 0.28 at 95% confidence level, assuming the Standard Model production cross section."
}
] | 2016A&A...593A.130H |
ATLAS detector | [
"ATLAS"
] | facility | used | high | [
{
"is_quantitative": true,
"text": "Recorded 20.3 fb^{-1} of proton-proton collision data at a centre-of-mass energy of 8 TeV at the LHC."
}
] | 2016A&A...593A.130H |
Higgs-portal dark matter | [] | concept | subject | medium | [
{
"is_quantitative": false,
"text": "The branching fraction limit of H to invisible particles is converted into upper bounds on the dark-matter-nucleon scattering cross section as a function of the dark-matter particle mass."
}
] | 2016A&A...593A.130H |
LHC | [] | facility | used | low | [] | 2016A&A...593A.130H |
star-forming galaxies | [
"SFGs"
] | concept | subject | high | [
{
"is_quantitative": true,
"text": "Massive star-forming galaxies at z = 2.2-2.5 commonly exhibit extremely compact dust emission with R_1/2,870 μm < 1.5 kpc, which is more than a factor of 2 smaller than their rest-optical sizes."
},
{
"is_quantitative": true,
"text": "These galaxies have high ... | 2017AcA....67...51R |
Atacama Large Millimeter/submillimeter Array | [
"ALMA"
] | facility | used | medium | [] | 2017AcA....67...51R |
quiescent galaxies | [] | concept | compared | medium | [
{
"is_quantitative": false,
"text": "The rest-frame far-infrared sizes of massive star-forming galaxies at z = 2.2-2.5 are comparable with the optical sizes of massive quiescent galaxies at similar redshifts."
}
] | 2017AcA....67...51R |
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