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1 ne glass (with a barrier to tunneling of 1.4 electron volts).
2 and-gap energy than rutile (2.32 versus 3.00 electron volts).
3 measured apparent activation energy of 0.16 electron volt.
4 n is most pronounced at approximately 1 kilo-electron volt.
5 and lowest unoccupied orbitals of 0.4 to 0.9 electron volt.
6 f the spectrum, up to photon energies of 280 electron volts.
7 unction of Ag, Cu, and Au electrodes to 3.65 electron volts.
8 c-ray electron intensity down to ~10 x 10(6) electron volts.
9 relatively narrow absorber band gap of 1.55 electron volts.
10 ate cosmic rays to energies close to ~10(15) electron volts.
11 tween 2 x 10(8) electron volts and 3 x10(11) electron volts.
12 d is observed at energies from 0.2 to 6 kilo-electron volts.
13 small optical gap edge of approximately 2.2 electron volts.
14 ale reconnection-driven flows are just a few electron volts.
15 ted to very high energies of several million electron volts.
16 metal with a band width of approximately 0.5 electron volts.
17 ron volts) and an optical energy gap of 0.34 electron volts.
18 with adsorption energies between 0.2 and 3.5 electron volts.
19 emitted via synchrotron radiation from peta-electron-volt (10(15) electron volts) electrons in a reg
20 ssion electron microscope, we detected a 5.7-electron volt (2175 angstrom) feature in interstellar gr
24 m from the ultraviolet to more than 1.6 kilo-electron volts, allowing, in principle, the generation o
26 spectrum of pulsed emission between 100 mega-electron volts and 400 GeV is described by a broken powe
27 a magnitude of approximately 10 to 100 milli-electron volts and a nanotube radius (r) dependence of a
28 erate particles to energies exceeding 10(12) electron volts and are bright sources of very-high-energ
29 emiconductor with a discrete band gap of 1.9 electron volts and can be chemically oxidized to enhance
30 vated conductivity (activation energy, 0.054 electron volts) and an optical energy gap of 0.34 electr
31 have narrow energy gaps (between 0.2 and 2.0 electron volts) and low densities, and they may be usefu
32 oximately 100 kilocalories per mole (about 4 electron volts) are reported for polyatomic molecules, i
33 band energy separation of approximately 0.25 electron volts, are capped by an epitaxial zinc selenide
34 termine the plasma frequency of 32.5 +/- 2.1 electron volts at a temperature of 5.5 kelvin, with a co
35 6 lines at 320, 400, 490, 560, 600, and 670 electron volts, attributable to electron capture and rad
37 in an energy splitting of more than 10 milli-electron volts between the K and K' valley exciton trans
38 ed to a difference of approximately 60 milli-electron volts between zero-point energies of incident p
39 tier of particle physics is several trillion electron volts, but colliders capable of reaching this r
41 ve and reveal a confinement gap of up to 0.5 electron volt, demonstrating the possibility of molecula
42 h ultrasharp peaks (widths of 12 to 25 milli-electron volts) devoid of the characteristic background
43 (Fig. 2C) as a function of maximum work (in electron volts) done by electron (laser photon) E(alpha)
44 on radiation from peta-electron-volt (10(15) electron volts) electrons in a region smaller than 1.4 x
45 87A) have resolved the 67.87- and 78.32-kilo-electron volt emission lines from decay of (44)Ti produc
46 f accelerated leptons, but the measured tera-electron volt emission profile constrains the diffusion
47 ent nonlinear optical spectroscopy with nano-electron volt energy resolution and low-temperature near
49 um perovskite cell optical band gap of ~1.75 electron volts (eV) can be achieved by varying halide co
50 This average temperature dependence (0.96 electron volts (eV)), which corresponds to a 57-fold inc
51 mma-ray (photon energy greater than 100 mega-electron volts) flares from this source detected by the
52 riable gamma-ray emission (0.1 to 10 billion electron volts) from the recently detected optical nova
53 erenkov Observatory (HAWC), of extended tera-electron volt gamma-ray emission coincident with the loc
54 m the Crab pulsar at energies above 100 giga-electron volts (GeV) with the Very Energetic Radiation I
55 ps reveal distinct nonthermal (0.2 to 6 kilo-electron volts) heliosheath proton populations with spec
57 graphite, it is found that changes of milli-electron volts in the energy range of up to 50 electron
58 stant is 1.62 per angstrom (the barrier, 2.6 electron volts) in a frozen 2-methyl-tetrahydrofuran gla
59 (and a broad resonance centered at +20 milli-electron volts) in spectroscopic measurements, indicatin
60 electrons with energies greater than 30 kilo-electron volts (keV) shortly after its insertion into or
61 e a gas-phase ionization energy (onset, 3.51 electron volts) lower than that of the cesium atom (whic
62 onths (radon exposure averaging 130,000 mega-electron volts of potential alpha energy per liter of ai
64 ay spectroscopy near the carbon K-edge ( 284 electron volts) on a tabletop apparatus to directly reve
65 ges that extend up to an energy of about 0.3 electron volt, or 40kTc (where k is the Boltzmann consta
68 th broad peaks from 10 x 10(6) to 40 x 10(6) electron volts per nucleon and an increasing galactic co
69 iron nuclei, with energies ~195 to ~500 mega-electron volts per nucleon, of which we identify 15 (60)
70 a of galactic cosmic rays down to ~3 x 10(6) electron volts per nucleon, revealing H and He energy sp
71 ge of energetic neutral atoms (ENAs) >6 kilo-electron volts produced by energetic protons occupying t
72 population comprises accelerated ions (<800 electron volts), produced upstream of Rosetta, and lower
74 endent of excitation photon energy over a ~1-electron volt range, and dependent on the excitation pol
75 ectron volts in the energy range of up to 50 electron volts reveal the compression and expansion of l
76 cluded HPLC-MS, Raman spectroscopy, and mega-electron volt-secondary ionization mass spectrometry.
77 interstellar modulation of high-energy (tera-electron volts, TeV) cosmic rays and diffusive propagati
78 ndence of the desorption yield peaks at 0.26 electron volt: the energy of the Si-H vibrational stretc
79 etic particles were observed up to 200 kilo--electron volts; these particles are capable of penetrati
80 n energy distribution width of less than 0.5 electron volts, this source of monochromatic electrons m
81 ral atoms (ENAs) at energies between tens of electron volts to hundreds of kiloelectron volts (keV).
82 idence for neutron emission near 2.5 million electron volts was also observed, as would be expected f
83 laser excitation (at a photon energy of 1.5 electron volts) was used to introduce a spatially period
84 tals of the carbon-atom framework, above 3.5 electron volts we found atomlike orbitals bound to the c
85 surface with electrons with an energy of 300 electron volts were analyzed by scanning tunneling micro
86 tron energies reach hundreds of thousands of electron volts, whereas the typical electron energies as
87 ission extending to high energies (>10 kilo--electron volts), which is ascribed to an accretion disk
88 mass-splitting with an accuracy of 300 kilo-electron volts, which is greater than 0 by 5 standard de
90 f conventional spin resonance (here ~10 nano-electron volts) with scanning tunneling microscopy to me
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