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Optical Measurement of Photorecombination Time Delays 光复合延时的光学测量
Ultrafast Science Pub Date : 2021-04-02 DOI: 10.34133/ultrafastscience.0034
Chunmei Zhang, Graham G. Brown, D. Ko, P. Corkum
{"title":"Optical Measurement of Photorecombination Time Delays","authors":"Chunmei Zhang, Graham G. Brown, D. Ko, P. Corkum","doi":"10.34133/ultrafastscience.0034","DOIUrl":"https://doi.org/10.34133/ultrafastscience.0034","url":null,"abstract":"Recollision physics and attosecond pulse generation meld the precision of optics with collision physics. As a follow-up to our previous work, we reveal a new direction for the study of electronic structure and multielectron dynamics by exploiting the collision-physics nature of recollision. We show experimentally that, by perturbing recollision trajectories with an infrared field, photorecombination time delays can be measured entirely optically using the Cooper minimum in argon as an example. In doing so, we demonstrate the relationship between recollision trajectories and the transition moment coupling the ground and continuum states. In particular, we show that recollision trajectories are influenced by their parent ion, while it is commonly assumed they are not. Our work paves the way for the entirely optical measurement of ultrafast electron dynamics and photorecombination delays due to electronic structure, multielectron interaction, and strong-field driven dynamics in complex molecular systems and correlated solid-state systems.","PeriodicalId":268204,"journal":{"name":"Ultrafast Science","volume":"379 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"2021-04-02","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"124729488","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 0
High-Harmonic Generation and Correlated Electron Emission from Relativistic Plasma Mirrors at 1 kHz Repetition Rate 重复频率为1khz的相对论性等离子体镜的高谐波产生和相关电子发射
Ultrafast Science Pub Date : 2020-05-04 DOI: 10.34133/2022/9893418
S. Haessler, M. Ouillé, J. Kaur, M. Bocoum, F. Böhle, D. Levy, L. Daniault, A. Vernier, J. Faure, R. López-Martens
{"title":"High-Harmonic Generation and Correlated Electron Emission from Relativistic Plasma Mirrors at 1 kHz Repetition Rate","authors":"S. Haessler, M. Ouillé, J. Kaur, M. Bocoum, F. Böhle, D. Levy, L. Daniault, A. Vernier, J. Faure, R. López-Martens","doi":"10.34133/2022/9893418","DOIUrl":"https://doi.org/10.34133/2022/9893418","url":null,"abstract":"<jats:p>We report evidence for the first generation of XUV spectra from relativistic surface high-harmonic generation (SHHG) on plasma mirrors at a kilohertz repetition rate, emitted simultaneously with energetic electrons. SHHG spectra and electron angular distributions are measured as a function of the experimentally controlled plasma density gradient scale length <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" id=\"M1\"><mml:msub><mml:mrow><mml:mi>L</mml:mi></mml:mrow><mml:mrow><mml:mi>g</mml:mi></mml:mrow></mml:msub></mml:math> for three increasingly short and intense driving pulses: 24 fs and <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" id=\"M2\"><mml:msub><mml:mrow><mml:mi>a</mml:mi></mml:mrow><mml:mrow><mml:mn>0</mml:mn></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mn>1.1</mml:mn></mml:math>, 8 fs and <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" id=\"M3\"><mml:msub><mml:mrow><mml:mi>a</mml:mi></mml:mrow><mml:mrow><mml:mn>0</mml:mn></mml:mrow></mml:msub><mml:mo>=</mml:mo><mml:mn>1.6</mml:mn></mml:math>, and finally 4 fs and <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" id=\"M4\"><mml:msub><mml:mrow><mml:mi>a</mml:mi></mml:mrow><mml:mrow><mml:mn>0</mml:mn></mml:mrow></mml:msub><mml:mo>≈</mml:mo><mml:mn>2.1</mml:mn></mml:math>, where <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" id=\"M5\"><mml:msub><mml:mrow><mml:mi>a</mml:mi></mml:mrow><mml:mrow><mml:mn>0</mml:mn></mml:mrow></mml:msub></mml:math> is the peak vector potential normalized by <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" id=\"M6\"><mml:msub><mml:mrow><mml:mi>m</mml:mi></mml:mrow><mml:mrow><mml:mi>e</mml:mi></mml:mrow></mml:msub><mml:mi>c</mml:mi><mml:mo>/</mml:mo><mml:mi>e</mml:mi></mml:math> with the elementary charge <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" id=\"M7\"><mml:mi>e</mml:mi></mml:math>, the electron rest mass <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" id=\"M8\"><mml:msub><mml:mrow><mml:mi>m</mml:mi></mml:mrow><mml:mrow><mml:mi>e</mml:mi></mml:mrow></mml:msub></mml:math>, and the vacuum light velocity <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" id=\"M9\"><mml:mi>c</mml:mi></mml:math>. For all driver pulses, we observe correlated relativistic SHHG and electron emission in the range <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" id=\"M10\"><mml:msub><mml:mrow><mml:mi>L</mml:mi></mml:mrow><mml:mrow><mml:mi>g</mml:mi></mml:mrow></mml:msub><mml:mo>∈</mml:mo><mml:mfenced open=\"[\" close=\"]\"><mml:mrow><mml:mi>λ</mml:mi><mml:mo>/</mml:mo><mml:mn>20</mml:mn><mml:mo>,</mml:mo><mml:mi>λ</mml:mi><mml:mo>/</mml:mo><mml:mn>4</mml:mn></mml:mrow></mml:mfenced></mml:math>, with an optimum gradient scale length of <mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" id=\"M11\"><mml:msub><mml:mrow><mml:mi>L</mml:mi></mml:mrow><mml:mrow><mml:mi>g</mml:mi></mml:mrow></mml:msub><mml:mo>≈</mml:mo><mml:mi>λ</mml:mi><mml:mo>/</mml:mo><mml:mn>10</mml:mn></mml:math>. This universal optimal <mml:m","PeriodicalId":268204,"journal":{"name":"Ultrafast Science","volume":"09 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"2020-05-04","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"124463818","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 8
THz-Enhanced DC Ultrafast Electron Diffractometer 太赫兹增强型直流超快电子衍射仪
Ultrafast Science Pub Date : 1900-01-01 DOI: 10.34133/2021/9848526
Dongfang Zhang, T. Kroh, F. Ritzkowsky, T. Rohwer, M. Fakhari, H. Cankaya, A. Calendron, N. Matlis, F. Kärtner
{"title":"THz-Enhanced DC Ultrafast Electron Diffractometer","authors":"Dongfang Zhang, T. Kroh, F. Ritzkowsky, T. Rohwer, M. Fakhari, H. Cankaya, A. Calendron, N. Matlis, F. Kärtner","doi":"10.34133/2021/9848526","DOIUrl":"https://doi.org/10.34133/2021/9848526","url":null,"abstract":"Terahertz- (THz-) based electron manipulation has recently been shown to hold tremendous promise as a technology for manipulating and driving the next generation of compact ultrafast electron sources. Here, we demonstrate an ultrafast electron diffractometer with THz-driven pulse compression. The electron bunches from a conventional DC gun are compressed by a factor of 10 and reach a duration of ~180 fs (FWHM) with 10,000 electrons/pulse at a 1 kHz repetition rate. The resulting ultrafast electron source is used in a proof-of-principle experiment to probe the photoinduced dynamics of single-crystal silicon. The THz-compressed electron beams produce high-quality diffraction patterns and enable the observation of the ultrafast structural dynamics with improved time resolution. These results validate the maturity of THz-driven ultrafast electron sources for use in precision applications.","PeriodicalId":268204,"journal":{"name":"Ultrafast Science","volume":"6 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"1900-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"122334534","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 11
Polarization Flipping of Even-Order Harmonics in Monolayer Transition-Metal Dichalcogenides 单层过渡金属二硫族化合物偶次谐波的极化翻转
Ultrafast Science Pub Date : 1900-01-01 DOI: 10.34133/2021/9820716
Yuki Kobayashi, C. Heide, Hamed Koochaki Kelardeh, Amalya C. Johnson, Fang Liu, T. Heinz, D. Reis, S. Ghimire
{"title":"Polarization Flipping of Even-Order Harmonics in Monolayer Transition-Metal Dichalcogenides","authors":"Yuki Kobayashi, C. Heide, Hamed Koochaki Kelardeh, Amalya C. Johnson, Fang Liu, T. Heinz, D. Reis, S. Ghimire","doi":"10.34133/2021/9820716","DOIUrl":"https://doi.org/10.34133/2021/9820716","url":null,"abstract":"We present a systematic study of the crystal-orientation dependence of high-harmonic generation in monolayer transition-metal dichalcogenides, WS2 and MoSe2, subjected to intense linearly polarized midinfrared laser fields. The measured spectra consist of both odd- and even-order harmonics, with a high-energy cutoff extending beyond the 15th order for a laser-field strength around ~1 V/nm. In WS2, we find that the polarization direction of the odd-order harmonics smoothly follows that of the laser field irrespective of the crystal orientation, whereas the direction of the even-order harmonics is fixed by the crystal mirror planes. Furthermore, the polarization of the even-order harmonics shows a flip in the course of crystal rotation when the laser field lies between two of the crystal mirror planes. By numerically solving the semiconductor Bloch equations for a gapped-graphene model, we qualitatively reproduce these experimental features and find the polarization flipping to be associated with a significant contribution from interband polarization. In contrast, high-harmonic signals from MoSe2 exhibit deviations from the laser-field following of odd-order harmonics and crystal-mirror-plane following of even-order harmonics. We attribute these differences to the competing roles of the intraband and interband contributions, including the deflection of the electron-hole trajectories by nonparabolic crystal bands.","PeriodicalId":268204,"journal":{"name":"Ultrafast Science","volume":"52 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"1900-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"130784445","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 28
Focusing Properties of High-Order Harmonics 高次谐波的聚焦特性
Ultrafast Science Pub Date : 1900-01-01 DOI: 10.34133/2021/9797453
M. Hoflund, J. Peschel, M. Plach, H. Dacasa, K. Veyrinas, E. Constant, P. Smorenburg, H. Wikmark, S. Maclot, Chen Guo, C. Arnold, A. L’Huillier, P. Eng-Johnsson
{"title":"Focusing Properties of High-Order Harmonics","authors":"M. Hoflund, J. Peschel, M. Plach, H. Dacasa, K. Veyrinas, E. Constant, P. Smorenburg, H. Wikmark, S. Maclot, Chen Guo, C. Arnold, A. L’Huillier, P. Eng-Johnsson","doi":"10.34133/2021/9797453","DOIUrl":"https://doi.org/10.34133/2021/9797453","url":null,"abstract":"Many applications of the extreme ultraviolet (XUV) radiation obtained by high-order harmonic generation (HHG) in gases require a small focus area in order to enable attosecond pulses to reach a high intensity. Here, high-order harmonics generated in Ar with a multiterawatt laser system in a loose focusing geometry are focused to a few micrometers using two toroidal mirrors in a Wolter configuration with a high demagnification factor. Using a knife-edge measurement technique, we determine the position and size of the XUV foci as a function of harmonic order. We show that the focus properties vary with harmonic order and the generation conditions. Simulations, based on a classical description of the harmonic dipole phase and assuming that the individual harmonics can be described as Gaussian beams, reproduce the experimental behavior. We discuss how the generation geometry affects the intensity and duration of the focused attosecond pulses.","PeriodicalId":268204,"journal":{"name":"Ultrafast Science","volume":"4 1","pages":"0"},"PeriodicalIF":0.0,"publicationDate":"1900-01-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"116020844","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":0,"RegionCategory":"","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
引用次数: 18
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