Quasidistribution of phases in Raman process with weak and strong pumps
Identifikátory výsledku
Kód výsledku v IS VaVaI
<a href="https://www.isvavai.cz/riv?ss=detail&h=RIV%2F61989592%3A15310%2F20%3A73600756" target="_blank" >RIV/61989592:15310/20:73600756 - isvavai.cz</a>
Výsledek na webu
<a href="https://iopscience.iop.org/article/10.1088/1402-4896/ab5316/pdf" target="_blank" >https://iopscience.iop.org/article/10.1088/1402-4896/ab5316/pdf</a>
DOI - Digital Object Identifier
<a href="http://dx.doi.org/10.1088/1402-4896/ab5316" target="_blank" >10.1088/1402-4896/ab5316</a>
Alternativní jazyky
Jazyk výsledku
angličtina
Název v původním jazyce
Quasidistribution of phases in Raman process with weak and strong pumps
Popis výsledku v původním jazyce
Nonclassicality is quantified using a quasidistribution of phases for the Raman process under both weak and strong pump conditions. In the former case, the solution is applicable to both resonant and off-resonant Raman processes, while strong classical pump is assumed at resonance. Under weak pump conditions (i.e. in a complete quantum treatment), the phase difference of phases described by single nonclassical modes is required to be filtered to describe a regular distribution function, which is not the case with strong pump. Compound Stokes-phonon mode shows nonclassical features of phases in both weak and strong pumping, which effect is similar to that for compound pump-phonon (Stokes-anti-Stokes) mode with weak (strong) pump. While anti-Stokes-phonon mode is observed to be classical and coherence conserving in strong pump case, pump-Stokes mode shows similar behavior in a special case in quantum treatment.
Název v anglickém jazyce
Quasidistribution of phases in Raman process with weak and strong pumps
Popis výsledku anglicky
Nonclassicality is quantified using a quasidistribution of phases for the Raman process under both weak and strong pump conditions. In the former case, the solution is applicable to both resonant and off-resonant Raman processes, while strong classical pump is assumed at resonance. Under weak pump conditions (i.e. in a complete quantum treatment), the phase difference of phases described by single nonclassical modes is required to be filtered to describe a regular distribution function, which is not the case with strong pump. Compound Stokes-phonon mode shows nonclassical features of phases in both weak and strong pumping, which effect is similar to that for compound pump-phonon (Stokes-anti-Stokes) mode with weak (strong) pump. While anti-Stokes-phonon mode is observed to be classical and coherence conserving in strong pump case, pump-Stokes mode shows similar behavior in a special case in quantum treatment.
Klasifikace
Druh
J<sub>imp</sub> - Článek v periodiku v databázi Web of Science
CEP obor
—
OECD FORD obor
10306 - Optics (including laser optics and quantum optics)
Návaznosti výsledku
Projekt
<a href="/cs/project/EF16_019%2F0000754" target="_blank" >EF16_019/0000754: Nanotechnologie pro budoucnost</a><br>
Návaznosti
P - Projekt vyzkumu a vyvoje financovany z verejnych zdroju (s odkazem do CEP)
Ostatní
Rok uplatnění
2020
Kód důvěrnosti údajů
S - Úplné a pravdivé údaje o projektu nepodléhají ochraně podle zvláštních právních předpisů
Údaje specifické pro druh výsledku
Název periodika
PHYSICA SCRIPTA
ISSN
0031-8949
e-ISSN
—
Svazek periodika
95
Číslo periodika v rámci svazku
3
Stát vydavatele periodika
SE - Švédské království
Počet stran výsledku
6
Strana od-do
"034001-1"-"034001-6"
Kód UT WoS článku
000509927300001
EID výsledku v databázi Scopus
2-s2.0-85079844967