Decoherence of the field in quantum nondemolition photon number measurement using the Kerr nonlinearity
Abstract The role of decoherence of an electromagnetic field in the process of quantum nondemolition measurement of the number of photons using a nonlinear Mach-Zehnder interferometer is investigated. This decoherence is caused by distributed losses in a Kerr medium. A long interaction time between...
Ausführliche Beschreibung
Autor*in: |
Kozlovskiĭ, A. V. [verfasserIn] |
---|
Format: |
Artikel |
---|---|
Sprache: |
Englisch |
Erschienen: |
2004 |
---|
Schlagwörter: |
---|
Anmerkung: |
© MAIK “Nauka/Interperiodica” 2004 |
---|
Übergeordnetes Werk: |
Enthalten in: Optics and spectroscopy - Nauka/Interperiodica, 1959, 97(2004), 5 vom: Nov., Seite 755-763 |
---|---|
Übergeordnetes Werk: |
volume:97 ; year:2004 ; number:5 ; month:11 ; pages:755-763 |
Links: |
---|
DOI / URN: |
10.1134/1.1828626 |
---|
Katalog-ID: |
OLC2047063833 |
---|
LEADER | 01000caa a22002652 4500 | ||
---|---|---|---|
001 | OLC2047063833 | ||
003 | DE-627 | ||
005 | 20230504105138.0 | ||
007 | tu | ||
008 | 200820s2004 xx ||||| 00| ||eng c | ||
024 | 7 | |a 10.1134/1.1828626 |2 doi | |
035 | |a (DE-627)OLC2047063833 | ||
035 | |a (DE-He213)1.1828626-p | ||
040 | |a DE-627 |b ger |c DE-627 |e rakwb | ||
041 | |a eng | ||
082 | 0 | 4 | |a 530 |q VZ |
084 | |a 11 |2 ssgn | ||
100 | 1 | |a Kozlovskiĭ, A. V. |e verfasserin |4 aut | |
245 | 1 | 0 | |a Decoherence of the field in quantum nondemolition photon number measurement using the Kerr nonlinearity |
264 | 1 | |c 2004 | |
336 | |a Text |b txt |2 rdacontent | ||
337 | |a ohne Hilfsmittel zu benutzen |b n |2 rdamedia | ||
338 | |a Band |b nc |2 rdacarrier | ||
500 | |a © MAIK “Nauka/Interperiodica” 2004 | ||
520 | |a Abstract The role of decoherence of an electromagnetic field in the process of quantum nondemolition measurement of the number of photons using a nonlinear Mach-Zehnder interferometer is investigated. This decoherence is caused by distributed losses in a Kerr medium. A long interaction time between the field and the medium is required to achieve a high accuracy in the photon number measurement. The losses in the Kerr medium accompanying the resonance four-wave interaction between the measured and the probe fields lead to a measurement error close to unity at γτ ≫1 (γ is the rate of losses in the medium, and τ is the time of interaction between the field and the medium); consequently, nondemolition quantum measurement turns out to be impossible in the scheme considered. Under these conditions, an increase in the intensity of the probe field does not result in achievement of the required measurement accuracy. | ||
650 | 4 | |a Quality Factor | |
650 | 4 | |a Photon Number | |
650 | 4 | |a Nonlinear Medium | |
650 | 4 | |a Fano Factor | |
650 | 4 | |a Splitting Plate | |
773 | 0 | 8 | |i Enthalten in |t Optics and spectroscopy |d Nauka/Interperiodica, 1959 |g 97(2004), 5 vom: Nov., Seite 755-763 |w (DE-627)129496499 |w (DE-600)207391-2 |w (DE-576)014895048 |x 0030-400X |7 nnns |
773 | 1 | 8 | |g volume:97 |g year:2004 |g number:5 |g month:11 |g pages:755-763 |
856 | 4 | 1 | |u https://doi.org/10.1134/1.1828626 |z lizenzpflichtig |3 Volltext |
912 | |a GBV_USEFLAG_A | ||
912 | |a SYSFLAG_A | ||
912 | |a GBV_OLC | ||
912 | |a SSG-OLC-PHY | ||
912 | |a GBV_ILN_21 | ||
912 | |a GBV_ILN_40 | ||
912 | |a GBV_ILN_60 | ||
912 | |a GBV_ILN_70 | ||
912 | |a GBV_ILN_170 | ||
912 | |a GBV_ILN_2004 | ||
912 | |a GBV_ILN_2014 | ||
912 | |a GBV_ILN_4116 | ||
951 | |a AR | ||
952 | |d 97 |j 2004 |e 5 |c 11 |h 755-763 |
author_variant |
a v k av avk |
---|---|
matchkey_str |
article:0030400X:2004----::eoeecoteiliqatmodmltopoonmemaueet |
hierarchy_sort_str |
2004 |
publishDate |
2004 |
allfields |
10.1134/1.1828626 doi (DE-627)OLC2047063833 (DE-He213)1.1828626-p DE-627 ger DE-627 rakwb eng 530 VZ 11 ssgn Kozlovskiĭ, A. V. verfasserin aut Decoherence of the field in quantum nondemolition photon number measurement using the Kerr nonlinearity 2004 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © MAIK “Nauka/Interperiodica” 2004 Abstract The role of decoherence of an electromagnetic field in the process of quantum nondemolition measurement of the number of photons using a nonlinear Mach-Zehnder interferometer is investigated. This decoherence is caused by distributed losses in a Kerr medium. A long interaction time between the field and the medium is required to achieve a high accuracy in the photon number measurement. The losses in the Kerr medium accompanying the resonance four-wave interaction between the measured and the probe fields lead to a measurement error close to unity at γτ ≫1 (γ is the rate of losses in the medium, and τ is the time of interaction between the field and the medium); consequently, nondemolition quantum measurement turns out to be impossible in the scheme considered. Under these conditions, an increase in the intensity of the probe field does not result in achievement of the required measurement accuracy. Quality Factor Photon Number Nonlinear Medium Fano Factor Splitting Plate Enthalten in Optics and spectroscopy Nauka/Interperiodica, 1959 97(2004), 5 vom: Nov., Seite 755-763 (DE-627)129496499 (DE-600)207391-2 (DE-576)014895048 0030-400X nnns volume:97 year:2004 number:5 month:11 pages:755-763 https://doi.org/10.1134/1.1828626 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_21 GBV_ILN_40 GBV_ILN_60 GBV_ILN_70 GBV_ILN_170 GBV_ILN_2004 GBV_ILN_2014 GBV_ILN_4116 AR 97 2004 5 11 755-763 |
spelling |
10.1134/1.1828626 doi (DE-627)OLC2047063833 (DE-He213)1.1828626-p DE-627 ger DE-627 rakwb eng 530 VZ 11 ssgn Kozlovskiĭ, A. V. verfasserin aut Decoherence of the field in quantum nondemolition photon number measurement using the Kerr nonlinearity 2004 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © MAIK “Nauka/Interperiodica” 2004 Abstract The role of decoherence of an electromagnetic field in the process of quantum nondemolition measurement of the number of photons using a nonlinear Mach-Zehnder interferometer is investigated. This decoherence is caused by distributed losses in a Kerr medium. A long interaction time between the field and the medium is required to achieve a high accuracy in the photon number measurement. The losses in the Kerr medium accompanying the resonance four-wave interaction between the measured and the probe fields lead to a measurement error close to unity at γτ ≫1 (γ is the rate of losses in the medium, and τ is the time of interaction between the field and the medium); consequently, nondemolition quantum measurement turns out to be impossible in the scheme considered. Under these conditions, an increase in the intensity of the probe field does not result in achievement of the required measurement accuracy. Quality Factor Photon Number Nonlinear Medium Fano Factor Splitting Plate Enthalten in Optics and spectroscopy Nauka/Interperiodica, 1959 97(2004), 5 vom: Nov., Seite 755-763 (DE-627)129496499 (DE-600)207391-2 (DE-576)014895048 0030-400X nnns volume:97 year:2004 number:5 month:11 pages:755-763 https://doi.org/10.1134/1.1828626 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_21 GBV_ILN_40 GBV_ILN_60 GBV_ILN_70 GBV_ILN_170 GBV_ILN_2004 GBV_ILN_2014 GBV_ILN_4116 AR 97 2004 5 11 755-763 |
allfields_unstemmed |
10.1134/1.1828626 doi (DE-627)OLC2047063833 (DE-He213)1.1828626-p DE-627 ger DE-627 rakwb eng 530 VZ 11 ssgn Kozlovskiĭ, A. V. verfasserin aut Decoherence of the field in quantum nondemolition photon number measurement using the Kerr nonlinearity 2004 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © MAIK “Nauka/Interperiodica” 2004 Abstract The role of decoherence of an electromagnetic field in the process of quantum nondemolition measurement of the number of photons using a nonlinear Mach-Zehnder interferometer is investigated. This decoherence is caused by distributed losses in a Kerr medium. A long interaction time between the field and the medium is required to achieve a high accuracy in the photon number measurement. The losses in the Kerr medium accompanying the resonance four-wave interaction between the measured and the probe fields lead to a measurement error close to unity at γτ ≫1 (γ is the rate of losses in the medium, and τ is the time of interaction between the field and the medium); consequently, nondemolition quantum measurement turns out to be impossible in the scheme considered. Under these conditions, an increase in the intensity of the probe field does not result in achievement of the required measurement accuracy. Quality Factor Photon Number Nonlinear Medium Fano Factor Splitting Plate Enthalten in Optics and spectroscopy Nauka/Interperiodica, 1959 97(2004), 5 vom: Nov., Seite 755-763 (DE-627)129496499 (DE-600)207391-2 (DE-576)014895048 0030-400X nnns volume:97 year:2004 number:5 month:11 pages:755-763 https://doi.org/10.1134/1.1828626 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_21 GBV_ILN_40 GBV_ILN_60 GBV_ILN_70 GBV_ILN_170 GBV_ILN_2004 GBV_ILN_2014 GBV_ILN_4116 AR 97 2004 5 11 755-763 |
allfieldsGer |
10.1134/1.1828626 doi (DE-627)OLC2047063833 (DE-He213)1.1828626-p DE-627 ger DE-627 rakwb eng 530 VZ 11 ssgn Kozlovskiĭ, A. V. verfasserin aut Decoherence of the field in quantum nondemolition photon number measurement using the Kerr nonlinearity 2004 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © MAIK “Nauka/Interperiodica” 2004 Abstract The role of decoherence of an electromagnetic field in the process of quantum nondemolition measurement of the number of photons using a nonlinear Mach-Zehnder interferometer is investigated. This decoherence is caused by distributed losses in a Kerr medium. A long interaction time between the field and the medium is required to achieve a high accuracy in the photon number measurement. The losses in the Kerr medium accompanying the resonance four-wave interaction between the measured and the probe fields lead to a measurement error close to unity at γτ ≫1 (γ is the rate of losses in the medium, and τ is the time of interaction between the field and the medium); consequently, nondemolition quantum measurement turns out to be impossible in the scheme considered. Under these conditions, an increase in the intensity of the probe field does not result in achievement of the required measurement accuracy. Quality Factor Photon Number Nonlinear Medium Fano Factor Splitting Plate Enthalten in Optics and spectroscopy Nauka/Interperiodica, 1959 97(2004), 5 vom: Nov., Seite 755-763 (DE-627)129496499 (DE-600)207391-2 (DE-576)014895048 0030-400X nnns volume:97 year:2004 number:5 month:11 pages:755-763 https://doi.org/10.1134/1.1828626 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_21 GBV_ILN_40 GBV_ILN_60 GBV_ILN_70 GBV_ILN_170 GBV_ILN_2004 GBV_ILN_2014 GBV_ILN_4116 AR 97 2004 5 11 755-763 |
allfieldsSound |
10.1134/1.1828626 doi (DE-627)OLC2047063833 (DE-He213)1.1828626-p DE-627 ger DE-627 rakwb eng 530 VZ 11 ssgn Kozlovskiĭ, A. V. verfasserin aut Decoherence of the field in quantum nondemolition photon number measurement using the Kerr nonlinearity 2004 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © MAIK “Nauka/Interperiodica” 2004 Abstract The role of decoherence of an electromagnetic field in the process of quantum nondemolition measurement of the number of photons using a nonlinear Mach-Zehnder interferometer is investigated. This decoherence is caused by distributed losses in a Kerr medium. A long interaction time between the field and the medium is required to achieve a high accuracy in the photon number measurement. The losses in the Kerr medium accompanying the resonance four-wave interaction between the measured and the probe fields lead to a measurement error close to unity at γτ ≫1 (γ is the rate of losses in the medium, and τ is the time of interaction between the field and the medium); consequently, nondemolition quantum measurement turns out to be impossible in the scheme considered. Under these conditions, an increase in the intensity of the probe field does not result in achievement of the required measurement accuracy. Quality Factor Photon Number Nonlinear Medium Fano Factor Splitting Plate Enthalten in Optics and spectroscopy Nauka/Interperiodica, 1959 97(2004), 5 vom: Nov., Seite 755-763 (DE-627)129496499 (DE-600)207391-2 (DE-576)014895048 0030-400X nnns volume:97 year:2004 number:5 month:11 pages:755-763 https://doi.org/10.1134/1.1828626 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_21 GBV_ILN_40 GBV_ILN_60 GBV_ILN_70 GBV_ILN_170 GBV_ILN_2004 GBV_ILN_2014 GBV_ILN_4116 AR 97 2004 5 11 755-763 |
language |
English |
source |
Enthalten in Optics and spectroscopy 97(2004), 5 vom: Nov., Seite 755-763 volume:97 year:2004 number:5 month:11 pages:755-763 |
sourceStr |
Enthalten in Optics and spectroscopy 97(2004), 5 vom: Nov., Seite 755-763 volume:97 year:2004 number:5 month:11 pages:755-763 |
format_phy_str_mv |
Article |
institution |
findex.gbv.de |
topic_facet |
Quality Factor Photon Number Nonlinear Medium Fano Factor Splitting Plate |
dewey-raw |
530 |
isfreeaccess_bool |
false |
container_title |
Optics and spectroscopy |
authorswithroles_txt_mv |
Kozlovskiĭ, A. V. @@aut@@ |
publishDateDaySort_date |
2004-11-01T00:00:00Z |
hierarchy_top_id |
129496499 |
dewey-sort |
3530 |
id |
OLC2047063833 |
language_de |
englisch |
fullrecord |
<?xml version="1.0" encoding="UTF-8"?><collection xmlns="http://www.loc.gov/MARC21/slim"><record><leader>01000caa a22002652 4500</leader><controlfield tag="001">OLC2047063833</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20230504105138.0</controlfield><controlfield tag="007">tu</controlfield><controlfield tag="008">200820s2004 xx ||||| 00| ||eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1134/1.1828626</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)OLC2047063833</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-He213)1.1828626-p</subfield></datafield><datafield tag="040" ind1=" " ind2=" "><subfield code="a">DE-627</subfield><subfield code="b">ger</subfield><subfield code="c">DE-627</subfield><subfield code="e">rakwb</subfield></datafield><datafield tag="041" ind1=" " ind2=" "><subfield code="a">eng</subfield></datafield><datafield tag="082" ind1="0" ind2="4"><subfield code="a">530</subfield><subfield code="q">VZ</subfield></datafield><datafield tag="084" ind1=" " ind2=" "><subfield code="a">11</subfield><subfield code="2">ssgn</subfield></datafield><datafield tag="100" ind1="1" ind2=" "><subfield code="a">Kozlovskiĭ, A. V.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Decoherence of the field in quantum nondemolition photon number measurement using the Kerr nonlinearity</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2004</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">Text</subfield><subfield code="b">txt</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">ohne Hilfsmittel zu benutzen</subfield><subfield code="b">n</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Band</subfield><subfield code="b">nc</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="500" ind1=" " ind2=" "><subfield code="a">© MAIK “Nauka/Interperiodica” 2004</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract The role of decoherence of an electromagnetic field in the process of quantum nondemolition measurement of the number of photons using a nonlinear Mach-Zehnder interferometer is investigated. This decoherence is caused by distributed losses in a Kerr medium. A long interaction time between the field and the medium is required to achieve a high accuracy in the photon number measurement. The losses in the Kerr medium accompanying the resonance four-wave interaction between the measured and the probe fields lead to a measurement error close to unity at γτ ≫1 (γ is the rate of losses in the medium, and τ is the time of interaction between the field and the medium); consequently, nondemolition quantum measurement turns out to be impossible in the scheme considered. Under these conditions, an increase in the intensity of the probe field does not result in achievement of the required measurement accuracy.</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Quality Factor</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Photon Number</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Nonlinear Medium</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Fano Factor</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Splitting Plate</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">Enthalten in</subfield><subfield code="t">Optics and spectroscopy</subfield><subfield code="d">Nauka/Interperiodica, 1959</subfield><subfield code="g">97(2004), 5 vom: Nov., Seite 755-763</subfield><subfield code="w">(DE-627)129496499</subfield><subfield code="w">(DE-600)207391-2</subfield><subfield code="w">(DE-576)014895048</subfield><subfield code="x">0030-400X</subfield><subfield code="7">nnns</subfield></datafield><datafield tag="773" ind1="1" ind2="8"><subfield code="g">volume:97</subfield><subfield code="g">year:2004</subfield><subfield code="g">number:5</subfield><subfield code="g">month:11</subfield><subfield code="g">pages:755-763</subfield></datafield><datafield tag="856" ind1="4" ind2="1"><subfield code="u">https://doi.org/10.1134/1.1828626</subfield><subfield code="z">lizenzpflichtig</subfield><subfield code="3">Volltext</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_USEFLAG_A</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SYSFLAG_A</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_OLC</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SSG-OLC-PHY</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_21</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_40</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_60</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_70</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_170</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2004</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2014</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4116</subfield></datafield><datafield tag="951" ind1=" " ind2=" "><subfield code="a">AR</subfield></datafield><datafield tag="952" ind1=" " ind2=" "><subfield code="d">97</subfield><subfield code="j">2004</subfield><subfield code="e">5</subfield><subfield code="c">11</subfield><subfield code="h">755-763</subfield></datafield></record></collection>
|
author |
Kozlovskiĭ, A. V. |
spellingShingle |
Kozlovskiĭ, A. V. ddc 530 ssgn 11 misc Quality Factor misc Photon Number misc Nonlinear Medium misc Fano Factor misc Splitting Plate Decoherence of the field in quantum nondemolition photon number measurement using the Kerr nonlinearity |
authorStr |
Kozlovskiĭ, A. V. |
ppnlink_with_tag_str_mv |
@@773@@(DE-627)129496499 |
format |
Article |
dewey-ones |
530 - Physics |
delete_txt_mv |
keep |
author_role |
aut |
collection |
OLC |
remote_str |
false |
illustrated |
Not Illustrated |
issn |
0030-400X |
topic_title |
530 VZ 11 ssgn Decoherence of the field in quantum nondemolition photon number measurement using the Kerr nonlinearity Quality Factor Photon Number Nonlinear Medium Fano Factor Splitting Plate |
topic |
ddc 530 ssgn 11 misc Quality Factor misc Photon Number misc Nonlinear Medium misc Fano Factor misc Splitting Plate |
topic_unstemmed |
ddc 530 ssgn 11 misc Quality Factor misc Photon Number misc Nonlinear Medium misc Fano Factor misc Splitting Plate |
topic_browse |
ddc 530 ssgn 11 misc Quality Factor misc Photon Number misc Nonlinear Medium misc Fano Factor misc Splitting Plate |
format_facet |
Aufsätze Gedruckte Aufsätze |
format_main_str_mv |
Text Zeitschrift/Artikel |
carriertype_str_mv |
nc |
hierarchy_parent_title |
Optics and spectroscopy |
hierarchy_parent_id |
129496499 |
dewey-tens |
530 - Physics |
hierarchy_top_title |
Optics and spectroscopy |
isfreeaccess_txt |
false |
familylinks_str_mv |
(DE-627)129496499 (DE-600)207391-2 (DE-576)014895048 |
title |
Decoherence of the field in quantum nondemolition photon number measurement using the Kerr nonlinearity |
ctrlnum |
(DE-627)OLC2047063833 (DE-He213)1.1828626-p |
title_full |
Decoherence of the field in quantum nondemolition photon number measurement using the Kerr nonlinearity |
author_sort |
Kozlovskiĭ, A. V. |
journal |
Optics and spectroscopy |
journalStr |
Optics and spectroscopy |
lang_code |
eng |
isOA_bool |
false |
dewey-hundreds |
500 - Science |
recordtype |
marc |
publishDateSort |
2004 |
contenttype_str_mv |
txt |
container_start_page |
755 |
author_browse |
Kozlovskiĭ, A. V. |
container_volume |
97 |
class |
530 VZ 11 ssgn |
format_se |
Aufsätze |
author-letter |
Kozlovskiĭ, A. V. |
doi_str_mv |
10.1134/1.1828626 |
dewey-full |
530 |
title_sort |
decoherence of the field in quantum nondemolition photon number measurement using the kerr nonlinearity |
title_auth |
Decoherence of the field in quantum nondemolition photon number measurement using the Kerr nonlinearity |
abstract |
Abstract The role of decoherence of an electromagnetic field in the process of quantum nondemolition measurement of the number of photons using a nonlinear Mach-Zehnder interferometer is investigated. This decoherence is caused by distributed losses in a Kerr medium. A long interaction time between the field and the medium is required to achieve a high accuracy in the photon number measurement. The losses in the Kerr medium accompanying the resonance four-wave interaction between the measured and the probe fields lead to a measurement error close to unity at γτ ≫1 (γ is the rate of losses in the medium, and τ is the time of interaction between the field and the medium); consequently, nondemolition quantum measurement turns out to be impossible in the scheme considered. Under these conditions, an increase in the intensity of the probe field does not result in achievement of the required measurement accuracy. © MAIK “Nauka/Interperiodica” 2004 |
abstractGer |
Abstract The role of decoherence of an electromagnetic field in the process of quantum nondemolition measurement of the number of photons using a nonlinear Mach-Zehnder interferometer is investigated. This decoherence is caused by distributed losses in a Kerr medium. A long interaction time between the field and the medium is required to achieve a high accuracy in the photon number measurement. The losses in the Kerr medium accompanying the resonance four-wave interaction between the measured and the probe fields lead to a measurement error close to unity at γτ ≫1 (γ is the rate of losses in the medium, and τ is the time of interaction between the field and the medium); consequently, nondemolition quantum measurement turns out to be impossible in the scheme considered. Under these conditions, an increase in the intensity of the probe field does not result in achievement of the required measurement accuracy. © MAIK “Nauka/Interperiodica” 2004 |
abstract_unstemmed |
Abstract The role of decoherence of an electromagnetic field in the process of quantum nondemolition measurement of the number of photons using a nonlinear Mach-Zehnder interferometer is investigated. This decoherence is caused by distributed losses in a Kerr medium. A long interaction time between the field and the medium is required to achieve a high accuracy in the photon number measurement. The losses in the Kerr medium accompanying the resonance four-wave interaction between the measured and the probe fields lead to a measurement error close to unity at γτ ≫1 (γ is the rate of losses in the medium, and τ is the time of interaction between the field and the medium); consequently, nondemolition quantum measurement turns out to be impossible in the scheme considered. Under these conditions, an increase in the intensity of the probe field does not result in achievement of the required measurement accuracy. © MAIK “Nauka/Interperiodica” 2004 |
collection_details |
GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_21 GBV_ILN_40 GBV_ILN_60 GBV_ILN_70 GBV_ILN_170 GBV_ILN_2004 GBV_ILN_2014 GBV_ILN_4116 |
container_issue |
5 |
title_short |
Decoherence of the field in quantum nondemolition photon number measurement using the Kerr nonlinearity |
url |
https://doi.org/10.1134/1.1828626 |
remote_bool |
false |
ppnlink |
129496499 |
mediatype_str_mv |
n |
isOA_txt |
false |
hochschulschrift_bool |
false |
doi_str |
10.1134/1.1828626 |
up_date |
2024-07-03T13:39:42.962Z |
_version_ |
1803565382197313536 |
fullrecord_marcxml |
<?xml version="1.0" encoding="UTF-8"?><collection xmlns="http://www.loc.gov/MARC21/slim"><record><leader>01000caa a22002652 4500</leader><controlfield tag="001">OLC2047063833</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20230504105138.0</controlfield><controlfield tag="007">tu</controlfield><controlfield tag="008">200820s2004 xx ||||| 00| ||eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1134/1.1828626</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)OLC2047063833</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-He213)1.1828626-p</subfield></datafield><datafield tag="040" ind1=" " ind2=" "><subfield code="a">DE-627</subfield><subfield code="b">ger</subfield><subfield code="c">DE-627</subfield><subfield code="e">rakwb</subfield></datafield><datafield tag="041" ind1=" " ind2=" "><subfield code="a">eng</subfield></datafield><datafield tag="082" ind1="0" ind2="4"><subfield code="a">530</subfield><subfield code="q">VZ</subfield></datafield><datafield tag="084" ind1=" " ind2=" "><subfield code="a">11</subfield><subfield code="2">ssgn</subfield></datafield><datafield tag="100" ind1="1" ind2=" "><subfield code="a">Kozlovskiĭ, A. V.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Decoherence of the field in quantum nondemolition photon number measurement using the Kerr nonlinearity</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2004</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">Text</subfield><subfield code="b">txt</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">ohne Hilfsmittel zu benutzen</subfield><subfield code="b">n</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Band</subfield><subfield code="b">nc</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="500" ind1=" " ind2=" "><subfield code="a">© MAIK “Nauka/Interperiodica” 2004</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract The role of decoherence of an electromagnetic field in the process of quantum nondemolition measurement of the number of photons using a nonlinear Mach-Zehnder interferometer is investigated. This decoherence is caused by distributed losses in a Kerr medium. A long interaction time between the field and the medium is required to achieve a high accuracy in the photon number measurement. The losses in the Kerr medium accompanying the resonance four-wave interaction between the measured and the probe fields lead to a measurement error close to unity at γτ ≫1 (γ is the rate of losses in the medium, and τ is the time of interaction between the field and the medium); consequently, nondemolition quantum measurement turns out to be impossible in the scheme considered. Under these conditions, an increase in the intensity of the probe field does not result in achievement of the required measurement accuracy.</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Quality Factor</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Photon Number</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Nonlinear Medium</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Fano Factor</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Splitting Plate</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">Enthalten in</subfield><subfield code="t">Optics and spectroscopy</subfield><subfield code="d">Nauka/Interperiodica, 1959</subfield><subfield code="g">97(2004), 5 vom: Nov., Seite 755-763</subfield><subfield code="w">(DE-627)129496499</subfield><subfield code="w">(DE-600)207391-2</subfield><subfield code="w">(DE-576)014895048</subfield><subfield code="x">0030-400X</subfield><subfield code="7">nnns</subfield></datafield><datafield tag="773" ind1="1" ind2="8"><subfield code="g">volume:97</subfield><subfield code="g">year:2004</subfield><subfield code="g">number:5</subfield><subfield code="g">month:11</subfield><subfield code="g">pages:755-763</subfield></datafield><datafield tag="856" ind1="4" ind2="1"><subfield code="u">https://doi.org/10.1134/1.1828626</subfield><subfield code="z">lizenzpflichtig</subfield><subfield code="3">Volltext</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_USEFLAG_A</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SYSFLAG_A</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_OLC</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SSG-OLC-PHY</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_21</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_40</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_60</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_70</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_170</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2004</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2014</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4116</subfield></datafield><datafield tag="951" ind1=" " ind2=" "><subfield code="a">AR</subfield></datafield><datafield tag="952" ind1=" " ind2=" "><subfield code="d">97</subfield><subfield code="j">2004</subfield><subfield code="e">5</subfield><subfield code="c">11</subfield><subfield code="h">755-763</subfield></datafield></record></collection>
|
score |
7.40102 |