{"title":"用于超短混沌量子光学的模型锁定热频梳","authors":"Kentaro Wakui, Yoshiaki Tsujimoto, Tadashi Kishimoto, Mikio Fujiwara, Masahide Sasaki, Aruto Hosaka, Fumihiko Kannari, Masahiro Takeoka","doi":"10.1002/qute.202400026","DOIUrl":null,"url":null,"abstract":"<p>Modelocked thermal frequency combs (MTCs) are generated by employing spectrally narrowed amplified spontaneous emission (ASE) seeded into an electro-optic frequency comb generator. The MTC emits 2-ps duration ultrashort pulses at a repetition rate of 10 GHz. Autocorrelation of the MTC pulses confirms a reduced coherence time, <span></span><math>\n <semantics>\n <mrow>\n <msub>\n <mi>τ</mi>\n <mi>c</mi>\n </msub>\n <mo>=</mo>\n <mn>213</mn>\n <mo>±</mo>\n <mn>16</mn>\n </mrow>\n <annotation>$\\tau _{\\mathrm{c}} = 213\\pm 16$</annotation>\n </semantics></math> ps, aligning with the narrowed bandwidth of the ASE seed. Intensity correlations of optically gated MTC pulses at a repetition rate of 250 MHz reveal nearly ideal thermal photon statistics with an experimental <span></span><math>\n <semantics>\n <mrow>\n <msubsup>\n <mi>g</mi>\n <mi>mtc</mi>\n <mrow>\n <mo>(</mo>\n <mn>2</mn>\n <mo>)</mo>\n </mrow>\n </msubsup>\n <mo>=</mo>\n <mn>1.9564</mn>\n <mo>±</mo>\n <mn>0.0004</mn>\n </mrow>\n <annotation>$g_{\\mathrm{mtc}}^{(2)} = 1.9564 \\pm 0.0004$</annotation>\n </semantics></math>, yielding an intrinsic <span></span><math>\n <semantics>\n <mrow>\n <msubsup>\n <mi>g</mi>\n <mi>int</mi>\n <mrow>\n <mo>(</mo>\n <mn>2</mn>\n <mo>)</mo>\n </mrow>\n </msubsup>\n <mo>=</mo>\n <mn>1.9809</mn>\n <mo>±</mo>\n <mn>0.0004</mn>\n </mrow>\n <annotation>$g_{\\mathrm{int}}^{(2)} = 1.9809 \\pm 0.0004$</annotation>\n </semantics></math> after background noise removal. As a practical application, second harmonic generation (SHG) is performed utilizing the optically gated MTC pulses as a pump and experimental intensity correlations, <span></span><math>\n <semantics>\n <msubsup>\n <mi>g</mi>\n <mi>sh</mi>\n <mrow>\n <mo>(</mo>\n <mn>2</mn>\n <mo>)</mo>\n </mrow>\n </msubsup>\n <annotation>$g_{\\mathrm{sh}}^{(2)}$</annotation>\n </semantics></math>, are examined for the SH photons. An entire transition in <span></span><math>\n <semantics>\n <msubsup>\n <mi>g</mi>\n <mi>sh</mi>\n <mrow>\n <mo>(</mo>\n <mn>2</mn>\n <mo>)</mo>\n </mrow>\n </msubsup>\n <annotation>$g_{\\mathrm{sh}}^{(2)}$</annotation>\n </semantics></math>, continuously changing from six to two by increasing the pump strength, agrees with the single-mode analytical model. Furthermore, time-resolved pulse height correlations allow to simultaneously acquire power variations in SHG and third harmonic generation against the pump. With the maximum peak intensity, <span></span><math>\n <semantics>\n <mrow>\n <msubsup>\n <mover>\n <mi>I</mi>\n <mo>¯</mo>\n </mover>\n <mn>1</mn>\n <mi>p</mi>\n </msubsup>\n <mo>≈</mo>\n <mn>1.6</mn>\n <mspace></mspace>\n <msup>\n <mrow>\n <mtext>GW</mtext>\n <mspace></mspace>\n <mtext>cm</mtext>\n </mrow>\n <mrow>\n <mo>−</mo>\n <mn>2</mn>\n </mrow>\n </msup>\n </mrow>\n <annotation>${\\overline{I}_{1}^{\\mathrm{p}}}\\approx 1.6 \\ {\\text{GW} \\ \\text{cm}}^{{-2}}$</annotation>\n </semantics></math>, realized in a periodically poled <span></span><math>\n <semantics>\n <msub>\n <mi>LiNbO</mi>\n <mn>3</mn>\n </msub>\n <annotation>${\\rm LiNbO}_3$</annotation>\n </semantics></math> waveguide for SHG, the demonstration highlights the potential for various applications in chaotic quantum optics experiments that necessitate ultrashort, high-intensity, single-spatiotemporal-mode thermal pulses.</p>","PeriodicalId":72073,"journal":{"name":"Advanced quantum technologies","volume":"8 2","pages":""},"PeriodicalIF":4.3000,"publicationDate":"2024-05-22","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://onlinelibrary.wiley.com/doi/epdf/10.1002/qute.202400026","citationCount":"0","resultStr":"{\"title\":\"Modelocked Thermal Frequency Combs for Ultrashort Chaotic Quantum Optics\",\"authors\":\"Kentaro Wakui, Yoshiaki Tsujimoto, Tadashi Kishimoto, Mikio Fujiwara, Masahide Sasaki, Aruto Hosaka, Fumihiko Kannari, Masahiro Takeoka\",\"doi\":\"10.1002/qute.202400026\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<p>Modelocked thermal frequency combs (MTCs) are generated by employing spectrally narrowed amplified spontaneous emission (ASE) seeded into an electro-optic frequency comb generator. The MTC emits 2-ps duration ultrashort pulses at a repetition rate of 10 GHz. Autocorrelation of the MTC pulses confirms a reduced coherence time, <span></span><math>\\n <semantics>\\n <mrow>\\n <msub>\\n <mi>τ</mi>\\n <mi>c</mi>\\n </msub>\\n <mo>=</mo>\\n <mn>213</mn>\\n <mo>±</mo>\\n <mn>16</mn>\\n </mrow>\\n <annotation>$\\\\tau _{\\\\mathrm{c}} = 213\\\\pm 16$</annotation>\\n </semantics></math> ps, aligning with the narrowed bandwidth of the ASE seed. Intensity correlations of optically gated MTC pulses at a repetition rate of 250 MHz reveal nearly ideal thermal photon statistics with an experimental <span></span><math>\\n <semantics>\\n <mrow>\\n <msubsup>\\n <mi>g</mi>\\n <mi>mtc</mi>\\n <mrow>\\n <mo>(</mo>\\n <mn>2</mn>\\n <mo>)</mo>\\n </mrow>\\n </msubsup>\\n <mo>=</mo>\\n <mn>1.9564</mn>\\n <mo>±</mo>\\n <mn>0.0004</mn>\\n </mrow>\\n <annotation>$g_{\\\\mathrm{mtc}}^{(2)} = 1.9564 \\\\pm 0.0004$</annotation>\\n </semantics></math>, yielding an intrinsic <span></span><math>\\n <semantics>\\n <mrow>\\n <msubsup>\\n <mi>g</mi>\\n <mi>int</mi>\\n <mrow>\\n <mo>(</mo>\\n <mn>2</mn>\\n <mo>)</mo>\\n </mrow>\\n </msubsup>\\n <mo>=</mo>\\n <mn>1.9809</mn>\\n <mo>±</mo>\\n <mn>0.0004</mn>\\n </mrow>\\n <annotation>$g_{\\\\mathrm{int}}^{(2)} = 1.9809 \\\\pm 0.0004$</annotation>\\n </semantics></math> after background noise removal. As a practical application, second harmonic generation (SHG) is performed utilizing the optically gated MTC pulses as a pump and experimental intensity correlations, <span></span><math>\\n <semantics>\\n <msubsup>\\n <mi>g</mi>\\n <mi>sh</mi>\\n <mrow>\\n <mo>(</mo>\\n <mn>2</mn>\\n <mo>)</mo>\\n </mrow>\\n </msubsup>\\n <annotation>$g_{\\\\mathrm{sh}}^{(2)}$</annotation>\\n </semantics></math>, are examined for the SH photons. An entire transition in <span></span><math>\\n <semantics>\\n <msubsup>\\n <mi>g</mi>\\n <mi>sh</mi>\\n <mrow>\\n <mo>(</mo>\\n <mn>2</mn>\\n <mo>)</mo>\\n </mrow>\\n </msubsup>\\n <annotation>$g_{\\\\mathrm{sh}}^{(2)}$</annotation>\\n </semantics></math>, continuously changing from six to two by increasing the pump strength, agrees with the single-mode analytical model. Furthermore, time-resolved pulse height correlations allow to simultaneously acquire power variations in SHG and third harmonic generation against the pump. With the maximum peak intensity, <span></span><math>\\n <semantics>\\n <mrow>\\n <msubsup>\\n <mover>\\n <mi>I</mi>\\n <mo>¯</mo>\\n </mover>\\n <mn>1</mn>\\n <mi>p</mi>\\n </msubsup>\\n <mo>≈</mo>\\n <mn>1.6</mn>\\n <mspace></mspace>\\n <msup>\\n <mrow>\\n <mtext>GW</mtext>\\n <mspace></mspace>\\n <mtext>cm</mtext>\\n </mrow>\\n <mrow>\\n <mo>−</mo>\\n <mn>2</mn>\\n </mrow>\\n </msup>\\n </mrow>\\n <annotation>${\\\\overline{I}_{1}^{\\\\mathrm{p}}}\\\\approx 1.6 \\\\ {\\\\text{GW} \\\\ \\\\text{cm}}^{{-2}}$</annotation>\\n </semantics></math>, realized in a periodically poled <span></span><math>\\n <semantics>\\n <msub>\\n <mi>LiNbO</mi>\\n <mn>3</mn>\\n </msub>\\n <annotation>${\\\\rm LiNbO}_3$</annotation>\\n </semantics></math> waveguide for SHG, the demonstration highlights the potential for various applications in chaotic quantum optics experiments that necessitate ultrashort, high-intensity, single-spatiotemporal-mode thermal pulses.</p>\",\"PeriodicalId\":72073,\"journal\":{\"name\":\"Advanced quantum technologies\",\"volume\":\"8 2\",\"pages\":\"\"},\"PeriodicalIF\":4.3000,\"publicationDate\":\"2024-05-22\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"https://onlinelibrary.wiley.com/doi/epdf/10.1002/qute.202400026\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Advanced quantum technologies\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://advanced.onlinelibrary.wiley.com/doi/10.1002/qute.202400026\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q1\",\"JCRName\":\"OPTICS\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Advanced quantum technologies","FirstCategoryId":"1085","ListUrlMain":"https://advanced.onlinelibrary.wiley.com/doi/10.1002/qute.202400026","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"OPTICS","Score":null,"Total":0}
Modelocked Thermal Frequency Combs for Ultrashort Chaotic Quantum Optics
Modelocked thermal frequency combs (MTCs) are generated by employing spectrally narrowed amplified spontaneous emission (ASE) seeded into an electro-optic frequency comb generator. The MTC emits 2-ps duration ultrashort pulses at a repetition rate of 10 GHz. Autocorrelation of the MTC pulses confirms a reduced coherence time, ps, aligning with the narrowed bandwidth of the ASE seed. Intensity correlations of optically gated MTC pulses at a repetition rate of 250 MHz reveal nearly ideal thermal photon statistics with an experimental , yielding an intrinsic after background noise removal. As a practical application, second harmonic generation (SHG) is performed utilizing the optically gated MTC pulses as a pump and experimental intensity correlations, , are examined for the SH photons. An entire transition in , continuously changing from six to two by increasing the pump strength, agrees with the single-mode analytical model. Furthermore, time-resolved pulse height correlations allow to simultaneously acquire power variations in SHG and third harmonic generation against the pump. With the maximum peak intensity, , realized in a periodically poled waveguide for SHG, the demonstration highlights the potential for various applications in chaotic quantum optics experiments that necessitate ultrashort, high-intensity, single-spatiotemporal-mode thermal pulses.