Single 10-fs deep-ultraviolet pulses generated by broadband four-wave mixing and high-order dispersion compensation
Abstract Broadband chirped-pulse four-wave mixing and a pulse compressor consisting of a prism pair and a grating pair are used to generate 10.3-fs deep-ultraviolet pulses. A large proportion of the dispersion up to 1000 $ fs^{2} $ is compensated without inducing third-order dispersion, which togeth...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Kida, Y. [verfasserIn] |
|---|
| Format: |
Artikel |
|---|---|
| Sprache: |
Englisch |
| Erschienen: |
2011 |
|---|
| Schlagwörter: |
|---|
| Systematik: |
|
|---|
| Anmerkung: |
© Springer-Verlag 2011 |
|---|
| Übergeordnetes Werk: |
Enthalten in: Applied physics. B, Lasers and optics - Springer-Verlag, 1981, 105(2011), 4 vom: 17. Nov., Seite 675-679 |
|---|---|
| Übergeordnetes Werk: |
volume:105 ; year:2011 ; number:4 ; day:17 ; month:11 ; pages:675-679 |
| Links: |
|---|
| DOI / URN: |
10.1007/s00340-011-4809-4 |
|---|
| Katalog-ID: |
OLC207430465X |
|---|
| LEADER | 01000caa a22002652 4500 | ||
|---|---|---|---|
| 001 | OLC207430465X | ||
| 003 | DE-627 | ||
| 005 | 20230331133341.0 | ||
| 007 | tu | ||
| 008 | 200819s2011 xx ||||| 00| ||eng c | ||
| 024 | 7 | |a 10.1007/s00340-011-4809-4 |2 doi | |
| 035 | |a (DE-627)OLC207430465X | ||
| 035 | |a (DE-He213)s00340-011-4809-4-p | ||
| 040 | |a DE-627 |b ger |c DE-627 |e rakwb | ||
| 041 | |a eng | ||
| 082 | 0 | 4 | |a 530 |a 620 |q VZ |
| 082 | 0 | 4 | |a 530 |q VZ |
| 084 | |a UA 9001 |q VZ |2 rvk | ||
| 100 | 1 | |a Kida, Y. |e verfasserin |4 aut | |
| 245 | 1 | 0 | |a Single 10-fs deep-ultraviolet pulses generated by broadband four-wave mixing and high-order dispersion compensation |
| 264 | 1 | |c 2011 | |
| 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 © Springer-Verlag 2011 | ||
| 520 | |a Abstract Broadband chirped-pulse four-wave mixing and a pulse compressor consisting of a prism pair and a grating pair are used to generate 10.3-fs deep-ultraviolet pulses. A large proportion of the dispersion up to 1000 $ fs^{2} $ is compensated without inducing third-order dispersion, which together with the smooth spectral and temporal profiles of the pulses makes them suitable for ultrafast spectroscopy. Unexpected spectral narrowing is observed when short input pulses were used for four-wave mixing. This narrowing is explained in terms of other third-order nonlinear phenomena, namely self-phase and cross-phase modulations, which occur simultaneously with four-wave mixing. | ||
| 650 | 4 | |a Hollow Fiber | |
| 650 | 4 | |a Pump Pulse | |
| 650 | 4 | |a Input Pulse | |
| 650 | 4 | |a Chirp Rate | |
| 650 | 4 | |a Frequency Chirp | |
| 700 | 1 | |a Liu, J. |4 aut | |
| 700 | 1 | |a Kobayashi, T. |4 aut | |
| 773 | 0 | 8 | |i Enthalten in |t Applied physics. B, Lasers and optics |d Springer-Verlag, 1981 |g 105(2011), 4 vom: 17. Nov., Seite 675-679 |w (DE-627)130297682 |w (DE-600)579693-3 |w (DE-576)015877272 |x 0946-2171 |7 nnns |
| 773 | 1 | 8 | |g volume:105 |g year:2011 |g number:4 |g day:17 |g month:11 |g pages:675-679 |
| 856 | 4 | 1 | |u https://doi.org/10.1007/s00340-011-4809-4 |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_22 | ||
| 912 | |a GBV_ILN_30 | ||
| 912 | |a GBV_ILN_60 | ||
| 912 | |a GBV_ILN_70 | ||
| 912 | |a GBV_ILN_130 | ||
| 912 | |a GBV_ILN_170 | ||
| 912 | |a GBV_ILN_285 | ||
| 912 | |a GBV_ILN_2018 | ||
| 912 | |a GBV_ILN_4036 | ||
| 912 | |a GBV_ILN_4116 | ||
| 912 | |a GBV_ILN_4126 | ||
| 912 | |a GBV_ILN_4266 | ||
| 912 | |a GBV_ILN_4277 | ||
| 912 | |a GBV_ILN_4313 | ||
| 912 | |a GBV_ILN_4323 | ||
| 936 | r | v | |a UA 9001 |
| 951 | |a AR | ||
| 952 | |d 105 |j 2011 |e 4 |b 17 |c 11 |h 675-679 | ||
| author_variant |
y k yk j l jl t k tk |
|---|---|
| matchkey_str |
article:09462171:2011----::ige0seplrvoeplegnrtdyrabnfuwvmxnadih |
| hierarchy_sort_str |
2011 |
| publishDate |
2011 |
| allfields |
10.1007/s00340-011-4809-4 doi (DE-627)OLC207430465X (DE-He213)s00340-011-4809-4-p DE-627 ger DE-627 rakwb eng 530 620 VZ 530 VZ UA 9001 VZ rvk Kida, Y. verfasserin aut Single 10-fs deep-ultraviolet pulses generated by broadband four-wave mixing and high-order dispersion compensation 2011 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer-Verlag 2011 Abstract Broadband chirped-pulse four-wave mixing and a pulse compressor consisting of a prism pair and a grating pair are used to generate 10.3-fs deep-ultraviolet pulses. A large proportion of the dispersion up to 1000 $ fs^{2} $ is compensated without inducing third-order dispersion, which together with the smooth spectral and temporal profiles of the pulses makes them suitable for ultrafast spectroscopy. Unexpected spectral narrowing is observed when short input pulses were used for four-wave mixing. This narrowing is explained in terms of other third-order nonlinear phenomena, namely self-phase and cross-phase modulations, which occur simultaneously with four-wave mixing. Hollow Fiber Pump Pulse Input Pulse Chirp Rate Frequency Chirp Liu, J. aut Kobayashi, T. aut Enthalten in Applied physics. B, Lasers and optics Springer-Verlag, 1981 105(2011), 4 vom: 17. Nov., Seite 675-679 (DE-627)130297682 (DE-600)579693-3 (DE-576)015877272 0946-2171 nnns volume:105 year:2011 number:4 day:17 month:11 pages:675-679 https://doi.org/10.1007/s00340-011-4809-4 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_21 GBV_ILN_22 GBV_ILN_30 GBV_ILN_60 GBV_ILN_70 GBV_ILN_130 GBV_ILN_170 GBV_ILN_285 GBV_ILN_2018 GBV_ILN_4036 GBV_ILN_4116 GBV_ILN_4126 GBV_ILN_4266 GBV_ILN_4277 GBV_ILN_4313 GBV_ILN_4323 UA 9001 AR 105 2011 4 17 11 675-679 |
| spelling |
10.1007/s00340-011-4809-4 doi (DE-627)OLC207430465X (DE-He213)s00340-011-4809-4-p DE-627 ger DE-627 rakwb eng 530 620 VZ 530 VZ UA 9001 VZ rvk Kida, Y. verfasserin aut Single 10-fs deep-ultraviolet pulses generated by broadband four-wave mixing and high-order dispersion compensation 2011 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer-Verlag 2011 Abstract Broadband chirped-pulse four-wave mixing and a pulse compressor consisting of a prism pair and a grating pair are used to generate 10.3-fs deep-ultraviolet pulses. A large proportion of the dispersion up to 1000 $ fs^{2} $ is compensated without inducing third-order dispersion, which together with the smooth spectral and temporal profiles of the pulses makes them suitable for ultrafast spectroscopy. Unexpected spectral narrowing is observed when short input pulses were used for four-wave mixing. This narrowing is explained in terms of other third-order nonlinear phenomena, namely self-phase and cross-phase modulations, which occur simultaneously with four-wave mixing. Hollow Fiber Pump Pulse Input Pulse Chirp Rate Frequency Chirp Liu, J. aut Kobayashi, T. aut Enthalten in Applied physics. B, Lasers and optics Springer-Verlag, 1981 105(2011), 4 vom: 17. Nov., Seite 675-679 (DE-627)130297682 (DE-600)579693-3 (DE-576)015877272 0946-2171 nnns volume:105 year:2011 number:4 day:17 month:11 pages:675-679 https://doi.org/10.1007/s00340-011-4809-4 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_21 GBV_ILN_22 GBV_ILN_30 GBV_ILN_60 GBV_ILN_70 GBV_ILN_130 GBV_ILN_170 GBV_ILN_285 GBV_ILN_2018 GBV_ILN_4036 GBV_ILN_4116 GBV_ILN_4126 GBV_ILN_4266 GBV_ILN_4277 GBV_ILN_4313 GBV_ILN_4323 UA 9001 AR 105 2011 4 17 11 675-679 |
| allfields_unstemmed |
10.1007/s00340-011-4809-4 doi (DE-627)OLC207430465X (DE-He213)s00340-011-4809-4-p DE-627 ger DE-627 rakwb eng 530 620 VZ 530 VZ UA 9001 VZ rvk Kida, Y. verfasserin aut Single 10-fs deep-ultraviolet pulses generated by broadband four-wave mixing and high-order dispersion compensation 2011 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer-Verlag 2011 Abstract Broadband chirped-pulse four-wave mixing and a pulse compressor consisting of a prism pair and a grating pair are used to generate 10.3-fs deep-ultraviolet pulses. A large proportion of the dispersion up to 1000 $ fs^{2} $ is compensated without inducing third-order dispersion, which together with the smooth spectral and temporal profiles of the pulses makes them suitable for ultrafast spectroscopy. Unexpected spectral narrowing is observed when short input pulses were used for four-wave mixing. This narrowing is explained in terms of other third-order nonlinear phenomena, namely self-phase and cross-phase modulations, which occur simultaneously with four-wave mixing. Hollow Fiber Pump Pulse Input Pulse Chirp Rate Frequency Chirp Liu, J. aut Kobayashi, T. aut Enthalten in Applied physics. B, Lasers and optics Springer-Verlag, 1981 105(2011), 4 vom: 17. Nov., Seite 675-679 (DE-627)130297682 (DE-600)579693-3 (DE-576)015877272 0946-2171 nnns volume:105 year:2011 number:4 day:17 month:11 pages:675-679 https://doi.org/10.1007/s00340-011-4809-4 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_21 GBV_ILN_22 GBV_ILN_30 GBV_ILN_60 GBV_ILN_70 GBV_ILN_130 GBV_ILN_170 GBV_ILN_285 GBV_ILN_2018 GBV_ILN_4036 GBV_ILN_4116 GBV_ILN_4126 GBV_ILN_4266 GBV_ILN_4277 GBV_ILN_4313 GBV_ILN_4323 UA 9001 AR 105 2011 4 17 11 675-679 |
| allfieldsGer |
10.1007/s00340-011-4809-4 doi (DE-627)OLC207430465X (DE-He213)s00340-011-4809-4-p DE-627 ger DE-627 rakwb eng 530 620 VZ 530 VZ UA 9001 VZ rvk Kida, Y. verfasserin aut Single 10-fs deep-ultraviolet pulses generated by broadband four-wave mixing and high-order dispersion compensation 2011 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer-Verlag 2011 Abstract Broadband chirped-pulse four-wave mixing and a pulse compressor consisting of a prism pair and a grating pair are used to generate 10.3-fs deep-ultraviolet pulses. A large proportion of the dispersion up to 1000 $ fs^{2} $ is compensated without inducing third-order dispersion, which together with the smooth spectral and temporal profiles of the pulses makes them suitable for ultrafast spectroscopy. Unexpected spectral narrowing is observed when short input pulses were used for four-wave mixing. This narrowing is explained in terms of other third-order nonlinear phenomena, namely self-phase and cross-phase modulations, which occur simultaneously with four-wave mixing. Hollow Fiber Pump Pulse Input Pulse Chirp Rate Frequency Chirp Liu, J. aut Kobayashi, T. aut Enthalten in Applied physics. B, Lasers and optics Springer-Verlag, 1981 105(2011), 4 vom: 17. Nov., Seite 675-679 (DE-627)130297682 (DE-600)579693-3 (DE-576)015877272 0946-2171 nnns volume:105 year:2011 number:4 day:17 month:11 pages:675-679 https://doi.org/10.1007/s00340-011-4809-4 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_21 GBV_ILN_22 GBV_ILN_30 GBV_ILN_60 GBV_ILN_70 GBV_ILN_130 GBV_ILN_170 GBV_ILN_285 GBV_ILN_2018 GBV_ILN_4036 GBV_ILN_4116 GBV_ILN_4126 GBV_ILN_4266 GBV_ILN_4277 GBV_ILN_4313 GBV_ILN_4323 UA 9001 AR 105 2011 4 17 11 675-679 |
| allfieldsSound |
10.1007/s00340-011-4809-4 doi (DE-627)OLC207430465X (DE-He213)s00340-011-4809-4-p DE-627 ger DE-627 rakwb eng 530 620 VZ 530 VZ UA 9001 VZ rvk Kida, Y. verfasserin aut Single 10-fs deep-ultraviolet pulses generated by broadband four-wave mixing and high-order dispersion compensation 2011 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Springer-Verlag 2011 Abstract Broadband chirped-pulse four-wave mixing and a pulse compressor consisting of a prism pair and a grating pair are used to generate 10.3-fs deep-ultraviolet pulses. A large proportion of the dispersion up to 1000 $ fs^{2} $ is compensated without inducing third-order dispersion, which together with the smooth spectral and temporal profiles of the pulses makes them suitable for ultrafast spectroscopy. Unexpected spectral narrowing is observed when short input pulses were used for four-wave mixing. This narrowing is explained in terms of other third-order nonlinear phenomena, namely self-phase and cross-phase modulations, which occur simultaneously with four-wave mixing. Hollow Fiber Pump Pulse Input Pulse Chirp Rate Frequency Chirp Liu, J. aut Kobayashi, T. aut Enthalten in Applied physics. B, Lasers and optics Springer-Verlag, 1981 105(2011), 4 vom: 17. Nov., Seite 675-679 (DE-627)130297682 (DE-600)579693-3 (DE-576)015877272 0946-2171 nnns volume:105 year:2011 number:4 day:17 month:11 pages:675-679 https://doi.org/10.1007/s00340-011-4809-4 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_21 GBV_ILN_22 GBV_ILN_30 GBV_ILN_60 GBV_ILN_70 GBV_ILN_130 GBV_ILN_170 GBV_ILN_285 GBV_ILN_2018 GBV_ILN_4036 GBV_ILN_4116 GBV_ILN_4126 GBV_ILN_4266 GBV_ILN_4277 GBV_ILN_4313 GBV_ILN_4323 UA 9001 AR 105 2011 4 17 11 675-679 |
| language |
English |
| source |
Enthalten in Applied physics. B, Lasers and optics 105(2011), 4 vom: 17. Nov., Seite 675-679 volume:105 year:2011 number:4 day:17 month:11 pages:675-679 |
| sourceStr |
Enthalten in Applied physics. B, Lasers and optics 105(2011), 4 vom: 17. Nov., Seite 675-679 volume:105 year:2011 number:4 day:17 month:11 pages:675-679 |
| format_phy_str_mv |
Article |
| institution |
findex.gbv.de |
| topic_facet |
Hollow Fiber Pump Pulse Input Pulse Chirp Rate Frequency Chirp |
| dewey-raw |
530 |
| isfreeaccess_bool |
false |
| container_title |
Applied physics. B, Lasers and optics |
| authorswithroles_txt_mv |
Kida, Y. @@aut@@ Liu, J. @@aut@@ Kobayashi, T. @@aut@@ |
| publishDateDaySort_date |
2011-11-17T00:00:00Z |
| hierarchy_top_id |
130297682 |
| dewey-sort |
3530 |
| id |
OLC207430465X |
| 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">OLC207430465X</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20230331133341.0</controlfield><controlfield tag="007">tu</controlfield><controlfield tag="008">200819s2011 xx ||||| 00| ||eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1007/s00340-011-4809-4</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)OLC207430465X</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-He213)s00340-011-4809-4-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="a">620</subfield><subfield code="q">VZ</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">UA 9001</subfield><subfield code="q">VZ</subfield><subfield code="2">rvk</subfield></datafield><datafield tag="100" ind1="1" ind2=" "><subfield code="a">Kida, Y.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Single 10-fs deep-ultraviolet pulses generated by broadband four-wave mixing and high-order dispersion compensation</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2011</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">© Springer-Verlag 2011</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract Broadband chirped-pulse four-wave mixing and a pulse compressor consisting of a prism pair and a grating pair are used to generate 10.3-fs deep-ultraviolet pulses. A large proportion of the dispersion up to 1000 $ fs^{2} $ is compensated without inducing third-order dispersion, which together with the smooth spectral and temporal profiles of the pulses makes them suitable for ultrafast spectroscopy. Unexpected spectral narrowing is observed when short input pulses were used for four-wave mixing. This narrowing is explained in terms of other third-order nonlinear phenomena, namely self-phase and cross-phase modulations, which occur simultaneously with four-wave mixing.</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Hollow Fiber</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Pump Pulse</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Input Pulse</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Chirp Rate</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Frequency Chirp</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Liu, J.</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Kobayashi, T.</subfield><subfield code="4">aut</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">Enthalten in</subfield><subfield code="t">Applied physics. B, Lasers and optics</subfield><subfield code="d">Springer-Verlag, 1981</subfield><subfield code="g">105(2011), 4 vom: 17. Nov., Seite 675-679</subfield><subfield code="w">(DE-627)130297682</subfield><subfield code="w">(DE-600)579693-3</subfield><subfield code="w">(DE-576)015877272</subfield><subfield code="x">0946-2171</subfield><subfield code="7">nnns</subfield></datafield><datafield tag="773" ind1="1" ind2="8"><subfield code="g">volume:105</subfield><subfield code="g">year:2011</subfield><subfield code="g">number:4</subfield><subfield code="g">day:17</subfield><subfield code="g">month:11</subfield><subfield code="g">pages:675-679</subfield></datafield><datafield tag="856" ind1="4" ind2="1"><subfield code="u">https://doi.org/10.1007/s00340-011-4809-4</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_22</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_30</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_130</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_285</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2018</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4036</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4116</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4126</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4266</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4277</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4313</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4323</subfield></datafield><datafield tag="936" ind1="r" ind2="v"><subfield code="a">UA 9001</subfield></datafield><datafield tag="951" ind1=" " ind2=" "><subfield code="a">AR</subfield></datafield><datafield tag="952" ind1=" " ind2=" "><subfield code="d">105</subfield><subfield code="j">2011</subfield><subfield code="e">4</subfield><subfield code="b">17</subfield><subfield code="c">11</subfield><subfield code="h">675-679</subfield></datafield></record></collection>
|
| author |
Kida, Y. |
| spellingShingle |
Kida, Y. ddc 530 rvk UA 9001 misc Hollow Fiber misc Pump Pulse misc Input Pulse misc Chirp Rate misc Frequency Chirp Single 10-fs deep-ultraviolet pulses generated by broadband four-wave mixing and high-order dispersion compensation |
| authorStr |
Kida, Y. |
| ppnlink_with_tag_str_mv |
@@773@@(DE-627)130297682 |
| format |
Article |
| dewey-ones |
530 - Physics 620 - Engineering & allied operations |
| delete_txt_mv |
keep |
| author_role |
aut aut aut |
| collection |
OLC |
| remote_str |
false |
| illustrated |
Not Illustrated |
| issn |
0946-2171 |
| topic_title |
530 620 VZ 530 VZ UA 9001 VZ rvk Single 10-fs deep-ultraviolet pulses generated by broadband four-wave mixing and high-order dispersion compensation Hollow Fiber Pump Pulse Input Pulse Chirp Rate Frequency Chirp |
| topic |
ddc 530 rvk UA 9001 misc Hollow Fiber misc Pump Pulse misc Input Pulse misc Chirp Rate misc Frequency Chirp |
| topic_unstemmed |
ddc 530 rvk UA 9001 misc Hollow Fiber misc Pump Pulse misc Input Pulse misc Chirp Rate misc Frequency Chirp |
| topic_browse |
ddc 530 rvk UA 9001 misc Hollow Fiber misc Pump Pulse misc Input Pulse misc Chirp Rate misc Frequency Chirp |
| format_facet |
Aufsätze Gedruckte Aufsätze |
| format_main_str_mv |
Text Zeitschrift/Artikel |
| carriertype_str_mv |
nc |
| hierarchy_parent_title |
Applied physics. B, Lasers and optics |
| hierarchy_parent_id |
130297682 |
| dewey-tens |
530 - Physics 620 - Engineering |
| hierarchy_top_title |
Applied physics. B, Lasers and optics |
| isfreeaccess_txt |
false |
| familylinks_str_mv |
(DE-627)130297682 (DE-600)579693-3 (DE-576)015877272 |
| title |
Single 10-fs deep-ultraviolet pulses generated by broadband four-wave mixing and high-order dispersion compensation |
| ctrlnum |
(DE-627)OLC207430465X (DE-He213)s00340-011-4809-4-p |
| title_full |
Single 10-fs deep-ultraviolet pulses generated by broadband four-wave mixing and high-order dispersion compensation |
| author_sort |
Kida, Y. |
| journal |
Applied physics. B, Lasers and optics |
| journalStr |
Applied physics. B, Lasers and optics |
| lang_code |
eng |
| isOA_bool |
false |
| dewey-hundreds |
500 - Science 600 - Technology |
| recordtype |
marc |
| publishDateSort |
2011 |
| contenttype_str_mv |
txt |
| container_start_page |
675 |
| author_browse |
Kida, Y. Liu, J. Kobayashi, T. |
| container_volume |
105 |
| class |
530 620 VZ 530 VZ UA 9001 VZ rvk |
| format_se |
Aufsätze |
| author-letter |
Kida, Y. |
| doi_str_mv |
10.1007/s00340-011-4809-4 |
| dewey-full |
530 620 |
| title_sort |
single 10-fs deep-ultraviolet pulses generated by broadband four-wave mixing and high-order dispersion compensation |
| title_auth |
Single 10-fs deep-ultraviolet pulses generated by broadband four-wave mixing and high-order dispersion compensation |
| abstract |
Abstract Broadband chirped-pulse four-wave mixing and a pulse compressor consisting of a prism pair and a grating pair are used to generate 10.3-fs deep-ultraviolet pulses. A large proportion of the dispersion up to 1000 $ fs^{2} $ is compensated without inducing third-order dispersion, which together with the smooth spectral and temporal profiles of the pulses makes them suitable for ultrafast spectroscopy. Unexpected spectral narrowing is observed when short input pulses were used for four-wave mixing. This narrowing is explained in terms of other third-order nonlinear phenomena, namely self-phase and cross-phase modulations, which occur simultaneously with four-wave mixing. © Springer-Verlag 2011 |
| abstractGer |
Abstract Broadband chirped-pulse four-wave mixing and a pulse compressor consisting of a prism pair and a grating pair are used to generate 10.3-fs deep-ultraviolet pulses. A large proportion of the dispersion up to 1000 $ fs^{2} $ is compensated without inducing third-order dispersion, which together with the smooth spectral and temporal profiles of the pulses makes them suitable for ultrafast spectroscopy. Unexpected spectral narrowing is observed when short input pulses were used for four-wave mixing. This narrowing is explained in terms of other third-order nonlinear phenomena, namely self-phase and cross-phase modulations, which occur simultaneously with four-wave mixing. © Springer-Verlag 2011 |
| abstract_unstemmed |
Abstract Broadband chirped-pulse four-wave mixing and a pulse compressor consisting of a prism pair and a grating pair are used to generate 10.3-fs deep-ultraviolet pulses. A large proportion of the dispersion up to 1000 $ fs^{2} $ is compensated without inducing third-order dispersion, which together with the smooth spectral and temporal profiles of the pulses makes them suitable for ultrafast spectroscopy. Unexpected spectral narrowing is observed when short input pulses were used for four-wave mixing. This narrowing is explained in terms of other third-order nonlinear phenomena, namely self-phase and cross-phase modulations, which occur simultaneously with four-wave mixing. © Springer-Verlag 2011 |
| collection_details |
GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_21 GBV_ILN_22 GBV_ILN_30 GBV_ILN_60 GBV_ILN_70 GBV_ILN_130 GBV_ILN_170 GBV_ILN_285 GBV_ILN_2018 GBV_ILN_4036 GBV_ILN_4116 GBV_ILN_4126 GBV_ILN_4266 GBV_ILN_4277 GBV_ILN_4313 GBV_ILN_4323 |
| container_issue |
4 |
| title_short |
Single 10-fs deep-ultraviolet pulses generated by broadband four-wave mixing and high-order dispersion compensation |
| url |
https://doi.org/10.1007/s00340-011-4809-4 |
| remote_bool |
false |
| author2 |
Liu, J. Kobayashi, T. |
| author2Str |
Liu, J. Kobayashi, T. |
| ppnlink |
130297682 |
| mediatype_str_mv |
n |
| isOA_txt |
false |
| hochschulschrift_bool |
false |
| doi_str |
10.1007/s00340-011-4809-4 |
| up_date |
2024-07-03T21:46:32.583Z |
| _version_ |
1803596010712203265 |
| 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">OLC207430465X</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20230331133341.0</controlfield><controlfield tag="007">tu</controlfield><controlfield tag="008">200819s2011 xx ||||| 00| ||eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1007/s00340-011-4809-4</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)OLC207430465X</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-He213)s00340-011-4809-4-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="a">620</subfield><subfield code="q">VZ</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">UA 9001</subfield><subfield code="q">VZ</subfield><subfield code="2">rvk</subfield></datafield><datafield tag="100" ind1="1" ind2=" "><subfield code="a">Kida, Y.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Single 10-fs deep-ultraviolet pulses generated by broadband four-wave mixing and high-order dispersion compensation</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2011</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">© Springer-Verlag 2011</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract Broadband chirped-pulse four-wave mixing and a pulse compressor consisting of a prism pair and a grating pair are used to generate 10.3-fs deep-ultraviolet pulses. A large proportion of the dispersion up to 1000 $ fs^{2} $ is compensated without inducing third-order dispersion, which together with the smooth spectral and temporal profiles of the pulses makes them suitable for ultrafast spectroscopy. Unexpected spectral narrowing is observed when short input pulses were used for four-wave mixing. This narrowing is explained in terms of other third-order nonlinear phenomena, namely self-phase and cross-phase modulations, which occur simultaneously with four-wave mixing.</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Hollow Fiber</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Pump Pulse</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Input Pulse</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Chirp Rate</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Frequency Chirp</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Liu, J.</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Kobayashi, T.</subfield><subfield code="4">aut</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">Enthalten in</subfield><subfield code="t">Applied physics. B, Lasers and optics</subfield><subfield code="d">Springer-Verlag, 1981</subfield><subfield code="g">105(2011), 4 vom: 17. Nov., Seite 675-679</subfield><subfield code="w">(DE-627)130297682</subfield><subfield code="w">(DE-600)579693-3</subfield><subfield code="w">(DE-576)015877272</subfield><subfield code="x">0946-2171</subfield><subfield code="7">nnns</subfield></datafield><datafield tag="773" ind1="1" ind2="8"><subfield code="g">volume:105</subfield><subfield code="g">year:2011</subfield><subfield code="g">number:4</subfield><subfield code="g">day:17</subfield><subfield code="g">month:11</subfield><subfield code="g">pages:675-679</subfield></datafield><datafield tag="856" ind1="4" ind2="1"><subfield code="u">https://doi.org/10.1007/s00340-011-4809-4</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_22</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_30</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_130</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_285</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_2018</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4036</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4116</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4126</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4266</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4277</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4313</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4323</subfield></datafield><datafield tag="936" ind1="r" ind2="v"><subfield code="a">UA 9001</subfield></datafield><datafield tag="951" ind1=" " ind2=" "><subfield code="a">AR</subfield></datafield><datafield tag="952" ind1=" " ind2=" "><subfield code="d">105</subfield><subfield code="j">2011</subfield><subfield code="e">4</subfield><subfield code="b">17</subfield><subfield code="c">11</subfield><subfield code="h">675-679</subfield></datafield></record></collection>
|
| score |
7.399417 |