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A given fluorophore may emit at single or multiple wavelengths (creatingan emission spectrum
when a sample of excited gas emits particular frequencies of light ATOMIC THEORY I. II(passive) is createdAn emission spectrum
excitation of ultraviolet lights in the compound(passive) caused bythe emission spectrum
excitation of ultraviolet lights in the BeBq2(passive) caused bythe emission spectrum
excitation of ultraviolet lights in the OXD-7(passive) caused bythe emission spectrum
excitation of ultraviolet lights in the Eu(TTA)3phen(passive) caused bythe emission spectrum
a third ring system ( Figures 4(c ) and 4(dinfluencesthe emission spectrum
a change in the potential difference between the first and second electrodes(passive) are caused bythe emission spectrum
Compositioninfluencesthe emission spectrum
Light is radiated by the Suncreatingan emission spectrum
atoms emitting photons of light(passive) are caused byEmission spectrum
heating or electrifying a gaswill createan emission spectrum
the drive current of the element(passive) caused byemission spectrum
the random spread of velocities in the gas(passive) caused bythe emission spectrum
rarefied gas emitting the(passive) is caused byan emission spectrum
Electrons Jumping in Atoms like the sun or stars like interstellar gas or a star 's atmosphere(passive) Caused bySpectrum - Absorbtion Emission
when a gas is heated and very specific wavelengths of light are produced(passive) is createdAn emission spectrum
when electrons of a hot gas fall from higher energy states to lower energy states , and emit a photon(passive) is createdAn emission spectrum
of ultraviolet and visible components(passive) is composedThe emission spectrum
the microwave(passive) caused byThe emission spectrum
the electrodes of HID lampsinfluencethe emission spectrum
the rotational transition of the atmospheric constituents(passive) caused byan emission spectrum
the atoms and ions within the plasma(passive) created byan emission spectrum
electron - hole recombination(passive) caused byemission spectrum
the analysis of their atomic spectrum(passive) were discovered bythe emission spectrum
any of the excitation light in the range of wavelengths 430nm~500 nm is irradiatedresultingemission spectrum
phase truncation(passive) caused bySpectrum emission
photoexcitation of the organic film O.sub.4(passive) caused bythe emission spectrum
this laboratory experimentwould createan emission spectrum
photoexcitation of the organic film O.sub.3(passive) caused bythe emission spectrum
electrons dropping to lower atomic energy states ... electromagnetic energy in the form of photons of light is given off in each transition downwards(passive) is caused byAn emission spectrum
the type of discharge gas to be filled(passive) can be set byThe emission spectrum
photoexcitation of the organic film O4(passive) caused bythe emission spectrum
photoexcitation of the organic film O3(passive) caused bythe emission spectrum
the x - ray tube voltage or the acceleration voltage with which the x - ray source is operated(passive) is decisively influenced byThe emission spectrum
TNH plasma(passive) caused bythe emission spectrum
of three peaks at 567 nm , 603 nm and 650 nm(passive) is composedEmission spectrum
the process by whichcreatesan emission spectrum
subjected to spectroscopic study i.e. high voltage dischargeto createan emission spectrum
a dense stellar wind caused by the extreme luminosity(passive) is created byThe emission spectrum
of the main emission linecomposedof the main emission line
Moreover , the excitation wavelength at the time of measuring(passive) was setMoreover , the excitation wavelength at the time of measuring
of a mixture of primary colors having imbalanced emission energy contentscomposedof a mixture of primary colors having imbalanced emission energy contents
from the decay of excited States of the material that transform with increasing frequency , eresultingfrom the decay of excited States of the material that transform with increasing frequency , e
Initial to true for the d state and false for the a statesetInitial to true for the d state and false for the a state
of a single line with photon energies from 1.26 to 1.55 eV ( 0.98 .mu.m tocomposedof a single line with photon energies from 1.26 to 1.55 eV ( 0.98 .mu.m to
substantially of narrow red , green and blue emission peaks ... and that the emission peaks in the spectrum of the nanophosphors in the left hand view of FIG . 2is composedsubstantially of narrow red , green and blue emission peaks ... and that the emission peaks in the spectrum of the nanophosphors in the left hand view of FIG . 2
from the energy transition between the levels 7 F1 A2 and 5 D0resultingfrom the energy transition between the levels 7 F1 A2 and 5 D0
from the transition between the levels 7 F1 A2 and 5 D0 depended on the angular frequency ωex of the excited lightresultingfrom the transition between the levels 7 F1 A2 and 5 D0 depended on the angular frequency ωex of the excited light
from the first emitting layer at the maximum luminescent wavelength and the luminescent intensity ( I2 ) of the emission spectrum originating from the second emitting layer at the maximum luminescent wavelengthoriginatingfrom the first emitting layer at the maximum luminescent wavelength and the luminescent intensity ( I2 ) of the emission spectrum originating from the second emitting layer at the maximum luminescent wavelength
from the excitation at various wavelengthsresultingfrom the excitation at various wavelengths
from excitation at 274 nmresultingfrom excitation at 274 nm
from X - ray excitationresultingfrom X - ray excitation
from the excitation of the final extractresultingfrom the excitation of the final extract
from excitation light with light of wavelengthresultingfrom excitation light with light of wavelength
from 458 nm excitation and the red traceresultingfrom 458 nm excitation and the red trace
from the impact excitation of H2 by a 30 eV electronresultingfrom the impact excitation of H2 by a 30 eV electron
a negative Stokes shift ... so its wavelength is shorter than that of excitation radiationcausesa negative Stokes shift ... so its wavelength is shorter than that of excitation radiation
independent of the excitation mode from 1PE to MPE like the quantum efficiencyresultsindependent of the excitation mode from 1PE to MPE like the quantum efficiency
upon excitation of the curable material system or of the article containing the cured material systemresultsupon excitation of the curable material system or of the article containing the cured material system
at an excitation peak wavelength ... and the monitoring wavelength at the time of measuring the excitation spectrum was set at the emission peak wavelengthwas setat an excitation peak wavelength ... and the monitoring wavelength at the time of measuring the excitation spectrum was set at the emission peak wavelength
from illumination of a substance ( usually a molecular gas ) by radiation of a definite frequency or definite frequenciesresultingfrom illumination of a substance ( usually a molecular gas ) by radiation of a definite frequency or definite frequencies
from the spectral gain function and longitudinal mode positions showncould resultfrom the spectral gain function and longitudinal mode positions shown
apparentlyoriginatesapparently
to the generation of characteristic emission spectral linesleadsto the generation of characteristic emission spectral lines
from an effectively narrow bandwidth transducer ( FIGresultingfrom an effectively narrow bandwidth transducer ( FIG
in a desired apparent color ... or to use multimode microcavities to obtain emission wavelengths which match a predetermined filter setto resultin a desired apparent color ... or to use multimode microcavities to obtain emission wavelengths which match a predetermined filter set
in white lightresultsin white light
at 254 nmwas setat 254 nm
from the extracted emission profileresultingfrom the extracted emission profile
of the photoluminescence of both A1Q and naphtho[2,3-a]pyrenecomposedof the photoluminescence of both A1Q and naphtho[2,3-a]pyrene
to a high CRImight contributeto a high CRI
from a photoluminescence test carried out at ambient temperature on a material of the inventionresultingfrom a photoluminescence test carried out at ambient temperature on a material of the invention
in stimulated Raman scattering cross - phase modulation ( SRS - XPMresultingin stimulated Raman scattering cross - phase modulation ( SRS - XPM
when an electron in an atom undergoes a transition from excited state to the ground stateresultswhen an electron in an atom undergoes a transition from excited state to the ground state
from excited electrons typically returning to their ground stateis createdfrom excited electrons typically returning to their ground state
of a mixture of primary colors each having an emission energy contentcomposedof a mixture of primary colors each having an emission energy content
of main emission lines of 3 nm or more and less than 10 nmcomposedof main emission lines of 3 nm or more and less than 10 nm
to increase of the threshold of old mode and decrease of the threshold 's intensityleadingto increase of the threshold of old mode and decrease of the threshold 's intensity
from the blendresultingfrom the blend