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阿秒钟技术为研究原子分子强场电离过程中电子超快动力学提供了强有力的工具。该技术依赖定量理论模型从实验测量得到的光电子频谱反演电离过程中系统的超快时域信息，而构建定量强场理论模型的关键问题之一是库仑效应的理论描述。与原子相比，分子具有多中心库仑势，在外场中具有许多新的效应，这为检验定量理论模型的适用性提供了更广阔平台。本文针对拉伸到大核间距的分子的阿秒钟特征观测量，比较了不同理论模型的预言，指出最近提出的半经典响应时间理论预言与数值实验结果更一致。该理论强调相较于具有经典性质的远核库仑效应，具有量子性质的近核库仑效应对分子隧穿电离影响更显著。本文进一步展望了该理论模型在具有电荷共振、固有偶极、取向效应以及复杂库仑势形式的分子强场电离中的应用。The attosecond technology provides a powerful tool for studying the ultrafast dynamics of electrons during the strong-field ionization of atoms and molecules. This technology relies on quantitative theoretical models to invert the ultrafast time-domain information of the system during the ionization process from the photoelectron spectrum obtained through experimental measurements. One of the key issues in constructing quantitative strong-field theoretical models is the theoretical description of the Coulomb effect. Compared with the single-center Coulomb potential of atoms, molecules have multi-center coulomb potential. This fundamental geometric structure feature leads to many new effects of molecules in the external field, such as orientation effect, charge resonance effect, intrinsic dipole effect and vibration effect. Therefore, it can be expected that the tunneling ionization process of molecules contains more phenomena than that of atoms, which is worthy of in-depth study by experiments and theories. Particularly for stretched molecular ions, such as H2+, those exhibiting charge resonance effects in external fields, the distinction between near-nucleus and far-nucleus Coulomb effects, which is of great significance for constructing quantitative theoretical models, becomes more complex, providing a platform for testing the applicability of quantitative theoretical models.
This work systematically compares the predictions of different theoretical models for the attoclock characteristic observables in molecular systems with large internuclear distances. Through comparative analysis, it is found that the recently proposed semiclassical response time theory, which incorporates near-nucleus Coulomb corrections, shows better agreement with numerical experimental results than the developed strong-field approximation models that consider far-nucleus Coulomb corrections. The semiclassical response time theory establishes a theoretical framework for describing strong-field ultrafast ionization dynamics of stretched molecular systems by considering dual-center Coulomb potential corrections and excited-state contributions. Specifically, it approximates the complex four-body interactions (electron-laser-dual nuclei) in stretched molecular systems into three-body interactions (electron-laser-dressed-up barrier-proximal nucleus), while incorporating the influence of the other nucleus on the potential barrier as a correction term for the tunnel-exit position. This framework highlights the significant impact of quantum-property-dominated near-nucleus Coulomb effects on molecular tunneling ionization. Furthermore, the theory provides an explicit formula for the response time determined by fundamental laser and molecular parameters. By calculating this response time, the theory deduces the values of attoclock observables, enabling a clear discussion of ionization time delays in stretched molecular tunneling ionization and revealing that such delays reflect the timescale of strong four-body interactions among the laser, electron, and molecular nuclei. In contrast, the developed strong-field approximation model that simultaneously accounts for excited-state effects and numerically solves Newtonian equations to describe far-nucleus Coulomb effects cannot fully describe the above-mentioned four-body interaction, making it difficult to quantitatively describe the complex tunneling ionization dynamics under the combined action of coulomb and excited states. Additionally, since this model cannot clearly define the ionization time, the related ionization time delay issues cannot be well discussed. Computational results demonstrate that the semi-classical response time theoretical model has improved both in terms of calculation accuracy and efficiency, thereby verifying the applicability of this theoretical model in the research process of molecular ultrafast ionization dynamics.
Moreover, for H2+ with intermediate internuclear distances, the charge resonance effect induces a significant ionization enhancement effect. We present relevant numerical experimental attoclock results and prospect the potential application of the response time theory in such systems. We also envision the extension of this theory to strong-field tunneling ionization in polar molecules, multi-center linear molecules, planar and three-dimensional molecules, and oriented molecules, where interference and Coulomb-acceleration effects compete. -
[1] Li W, Zhou X B, Lock R, Patchkovskii S, Stolow A, Kapteyn H C, Murnane M M 2008 Science 322 1207
[2] Krausz F, Ivanov M 2009 Rev. Mod. Phys. 81 163
[3] Lépine F, Ivanov M Y, Vrakking M J J 2014 Nat. Photon 8 195
[4] Garg M, Zhan M, Luu T T, Lakhotia H, Klostermann T, Guggenmos A, Goulielmakis E 2016 Nature 538 359
[5] Lakhotia H, Kim H Y, Zhan M, Hu S, Meng S, Goulielmakis E 2020 Nature 583 55
[6] MacColl L A 1932 Phys. Rev. 40 621
[7] Wigner E P 1955 Phys. Rev. 98 145
[8] Ranfagni A, Mugnai D, Fabeni P, Pazzi G P 1991 Appl Phys. Lett. 58 774
[9] Enders A, Nimtz G 1992 J. Phys. 12 1693
[10] Steinberg A M, Kwiat P G, Chiao R Y 1993 Phys. Rev. Lett. 71 708
[11] Spielmann C, Szipöcs R, Stingl A, Krausz F 1994 Phys. Rev. Lett. 73 2308
[12] Muga J G, Sala Mayato R, Egusquiza I L (eds.) 2002 Time in Quantum Mechanics (Vol. 1) (Berlin, Heidelberg: Springer) pp. 5–6
[13] Ramos R, Spierings D, Racicot I, Steinberg A M 2020 Nature 583 529
[14] Eckle P, Smolarski M, Schlup P, Biegert J, Staudte A, Schöffler M, Muller H G, Dörner R, Keller U 2008 Nat. Phys. 4 565
[15] Eckle P, Pfeiffer A N, Cirelli C, Staudte A, Dörner R, Muller H G, Buttiker M, Keller U 2008 Science 322 1525
[16] Pfeiffer A N, Cirelli C, Smolarski M, Dimitrovski D, Abu-samha M, Madsen L B, Keller U 2012 Nat. Phys. 8 76
[17] Pfeiffer A N, Cirelli C, Smolarski M, Keller U 2013 Chem. Phys. 414 84
[18] Landsman A S, Weger M, Maurer J, Boge R, Ludwig A, Heuser S, Cirelli C, Gallmann L, Keller U 2014 Optica 1 343
[19] Klaiber M, Hatsagortsyan K Z, Keitel C H 2015 Phys. Rev. Lett. 114 083001
[20] Hofmann C, Landsman A S, Kelle U 2019 J. Mod. Optic. 66 1052
[21] Serov V V, Bray A W, Kheifets A S 2019 Phys. Rev. A 99 063428
[22] Sainadh U S, Xu H, Wang X, Atia-Tul-Noor A, Wallace W C, Douguet N, Bray A W, Ivanov I, Bartschat K, Kheifets A, Sang R T, Litvinyuk I V 2019 Nature 568 75
[23] Chen C, Che J Y, Xie X J, Wang S, Xin G G, Chen Y J 2022 Chin. Phys. B 31 033201
[24] Che J Y, Chen C, Li W Y, Li W, Chen Y J 2023 Acta Phys. Sin. 72 193301
[25] Yan T M, Popruzhenko S V, Vrakking M J J, Bauer D 2010 Phys. Rev. Lett. 105 253002
[26] Li M, Geng J, Liu H, Deng Y K, Wu C Y, Peng L Y, Gong Q H, Liu Y Q 2014 Phys. Rev. Lett. 112 113002
[27] Lai X Y, Poli C, Schomerus H, Figueira de Morisson Faria C 2015 Phys. Rev. Lett. 92 043407
[28] Shvetsov-Shilovski N I, Lein M, Madsen L B, Räsänen E, Lemell C, Burgdörfer J, Arbó D G, Tőkési K 2016 Phys. Rev. A 94 013415
[29] Xie X, Chen C, Xin G, Liu J, Chen Y 2020 Opt. Express 28 33228
[30] Che J Y, Chen C, Li W Y, Wang S, Xie X J, Huang J Y, Peng Y G, Xin G G, Chen Y J 2022 arXiv:2111.08491
[31] Camus N, Yakaboylu E, Fechner L, Klaiber M, Laux M, Mi Y, Hatsagortsyan K Z, Pfeifer T, Keitel C H, Moshammer R 2017 Phys. Rev. Lett. 119 023201
[32] Chen Y J, Liu J, Hu B 2009 Phys. Rev. A 79 033405
[33] Frumker E, Hebeisen C T, Kajumba N, Bertrand J B, Wörner H J, Spanner M, Villeneuve D M, Naumov A, Corkum P B 2012 Phys. Rev. Lett. 109 233904
[34] Chen Y J, Zhang B 2012 J. Phys. B 45 215601
[35] Li W Y, Dong F L, Yu S J, Wang S, Yang S P, Chen Y J 2015 Opt. Express 23 031010
[36] Li W Y, Wang S, Shi Y Z, Yang S P, Chen Y J 2017 J. Phys. B 50 085003
[37] Wang S, Che J Y, Chen C, Xin G G, Chen Y J 2020 Phys. Rev. A 102 053103
[38] Etches A, Gaarde M B, Madsen L B 2012 Phys. Rev. A 86 023818
[39] Li W Y, Yu S J, Wang S, Chen Y J 2016 Phys. Rev. A 94 053407
[40] Shen S Q, Chen Z Y, Wang S, Che J Y, Chen Y J 2024 Phys. Rev. A 110 033106
[41] Brabec T, Ivanov M Yu, Corkum P B 1996 Phys. Rev. A 54 R2551
[42] Goreslavski S P, Paulus G G, Popruzhenko S V, Shvetsov-Shilovski N I 2004 Phys. Rev. Lett. 93 233002
[43] Feit M D, Fleck J A, Steiger A 1982 J. Comput. Phys. 47 412
[44] Lewenstein M, Kulander K C, Schafer K J, Bucksbaum P H 1995 Phys. Rev. A 51 1495
[45] Corkum P B, Krausz F 2007 Nat. Phys. 3 381
[46] Ren D, Wang S, Chen C, Li X, Yu X, Zhao X, Ma P, Wang C, Luo S, Chen Y, Ding D 2022 J. Phys. B 55 175101
[47] Becker W, Grasbon F, Kopold R, Milošević D B, Paulus G G, Walther H 2002 Adv. At. Mol. Opt. Phys. 48 35
[48] Chen Y J, Hu B 2010 Phys. Rev. A 81 013411
[49] Sun F J, Chen C, Li W Y, Liu X, Li W, Chen Y J 2021 Phys. Rev. A 103 053108
[50] Zuo T, Bandrauk A D 1995 Phys. Rev. A 52 R2511
[51] Becker W, Chen J, Chen S G, Milošević D B 2007 Phys. Rev. A 76 033403
[52] Che J Y, Zhang F B, Li W Y, Chen C, Chen Y J 2023 New J. Phys. 25 083022
[53] Chen J, Chen S G 2007 Phys. Rev. A 75 041402(R)
[54] Blaga C I, Catoire F, Colosimo P, Paulus G G, Muller H G, Agostini P, DiMauro L F 2009 Nat. Phys. 5 335
[55] Corkum P B 1993 Phys. Rev. Lett. 71 1994
[56] Yang B, Schafer K J, Walker B, Kulander K C, Agostini P, DiMauro L F 1993 Phys. Rev. Lett. 71 3770
[57] Peng Y G, Che J Y, Zhang F B, Xie X J, Xin G G, Chen Y J 2024 Opt. Express 32 12734
[58] Chen Z Y, Shen S Q, Li Y P, Yang Z Q, Che J Y, Chen Y J (unpublished)
[59] Chen Y J, Chen J, Liu J 2006 Phys. Rev. A 74 063405
[60] Kamta G L, Bandrauk A D 2005 Phys. Rev. Lett. 94 203003
[61] Shi Y Z, Zhang B, Yu W Y, Chen Y J 2017 Phys. Rev. A 95 033406
[62] Wang S, Cai J, Chen Y J 2017 Phys. Rev. A 96 043413
[63] Su N, Yu S J, Li W Y, Yang S P, Chen Y J 2018 Chin. Phys. B 27 054213
[64] Yu S J, Li W Y, Li Y P, Chen Y J 2017 Phys. Rev. A 96 013432
[65] Chen Y J, Hu Bambi 2009 J. Chem. Phys 131 244109
[66] Gao F, Chen Y J, Xin G G, Liu J, Fu L B 2017 Phys. Rev. A 96 063414
[67] Chen C, Ren D X, Han X, Yang S P, Chen Y J 2018 Phys. Rev. A 98 063425
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