Theory of Attosecond Phenomena

  • ISHIKAWA K
N/ACitations
Citations of this article
7Readers
Mendeley users who have this article in their library.

Abstract

Attosecond extreme ultraviolet and soft X-ray pulses are generated through high-order harmonic generation , a highly non-linear and non-perturbative phenomenon. Nonlinear optical effects and electron-electron interaction play an essential role in various applications of attosecond pulses. The best way to study atomic dynamics under such circumstances theoretically is direct numerical simulation of the time-dependent Schrodinger equation (TDSE). The present article introduces how to model the high-field and ultrafast phenomena on the basis of TDSE, and reviews recent theoretical findings on attosecond pulse generation and attosecond phenomena , peculiar to the time scale of electronic motion inside an atom. 1.•@ ‚Í ‚ ¶ ‚ß ‚É ‹É '[ Ž ‡ ŠO(XUV)‚¨‚ae‚¨‚ae ‚Ñ"îX•ü-Ì ˆae ‚Å‚Ì•V ‚µ‚¢•‚ ‹-"x '´ 'Z ƒp ƒ‹ ƒXOEõ OE¹ ‚Ì'ã •\ ‚AE ‚µ‚Ä•‚ ŽŸ •‚'² "g1)‚ª ‚ ‚° ‚ç‚ê ‚é .2001 "N ‚ÉKrausz‚ç ‚ª •‚ŽŸ •‚ '² "g "-• ¶(HHG)‚É ‚ae ‚èƒp ƒ‹ ƒX ••‚ª1 ƒtƒF ƒ€ ƒg•b ‚ð•Ø ‚é ƒA ƒg•b "î ƒG ƒbƒNƒX •ü ƒp ƒ‹ ƒX ‚Ì"-• ¶ ‚É•¬ OE÷ ‚µ,•¨ Ž¿ ' † ‚Ì"d Žq ‚Ì'´ •‚ '¬ ‰^ "® ‚ðŠÏ 'ª ‚µ‚½ ‚è Ž©-R ‚É'€ •ì ‚µ‚½ ‚è‚· ‚é•u ƒA ƒg •b ‰È Šw •v‚AE‚¢ ‚¤•V-Ì ˆae ‚ª'a • ¶ ‚µ‚½2).‚± ‚ê ‚ç‚Ì ‰ß 'ö ‚ð-• ˜_ "I ‚ÉOE¤ ‹ † ‚· ‚é ‚É ‚Í ‚Ç‚¤‚· ‚ê ‚Î ‚ae‚¢ ‚Ì ‚Å ‚ ‚ë ‚¤ ‚©.-Ê Žq OEn ‚Ì-•˜_ ‚AE‚¢ ‚¤ ‚AE'ae1OE´-ae1OE´-• OEv ŽZ ‚â-Ê Žq‰» Šw OEv ŽZ ‚ðŽv ‚¢ •‚ ‚© ‚× ‚é•l ‚à'½ ‚¢ ‚Å ‚ ‚ë ‚¤.‚µ ‚© ‚µ,•‚ ŽŸ •‚ '² "g "-• ¶ ‚Í •‚ "x ‚É"ñ •ü OE`OE`•E "ñ •Û "® ˜_ "I ‚È‰ß 'ö ‚Å ‚ ‚è,‚Ü ‚½ ƒA ƒg•b OE» •Û ‚Å ŠÖ •S ‚Ì "I ‚É ‚È ‚Á ‚Ä ‚¢ ‚é‚Ì ‚Í"d Žq 'Š ŠÖ‚ª •d-v ‚È-ð Š" ‚ð‰Ê ‚½ ‚· ƒ_ ƒC ƒi ƒ~ƒN ƒX ‚Å ‚ ‚邽 ‚ß,‚± ‚ê ‚ç‚ÌŽè-@ ‚Å ‚Í(OE» Žž "_ ‚Å ‚Í)‚¤ ‚Ü ‚-Žae ‚舵 ‚¤ ‚± ‚AE‚ª ‚Å ‚«‚È ‚¢. Šî-{ ‚É-§ ‚¿ •Ô ‚ê ‚Î,-Ê Žq OEn ‚Ì ƒ_ƒC ƒi ƒ~ ƒNƒX ‚Í,Žž ŠÔˆË ' ¶ ƒV ƒ… ƒOE•[ ƒf ƒB ƒ"ƒK •[•û 'ö Ž®(time-dependent Schrodinger equation, TDSE)‚É ‚ae ‚Á‚Ä OE´-OE´-• "I ‚É•³ Šm ‚É‹L •q ‚· ‚é ‚± ‚AE‚ª ‚Å ‚« ‚é.‚» ‚µ‚ÄOE» •Ý ‚Ü‚Å ‚Ì ‚AE‚± ‚ë•… 'f,ƒw ƒŠ ƒEƒ€,ƒŠ ƒ` ƒE ƒ€ ‚É ŠÖ ‚µ‚Ä ‚Í,•u OE´-OE´-• "I ‚É•v ‚Å ‚Í ‚È ‚-•u ŽÀ •Û ‚É•vTDSE‚É ‚ae ‚Á‚Ä ƒ_ ƒC ƒi ƒ~ƒN ƒX ‚ðOEv ŽZ ‚· ‚é ‚± ‚AE‚ª ‚Å ‚« ,•‚ ŽŸ •‚ '² "g "-• ¶ ‚â ƒA ƒg•b OE» •Û ‚ÍŽå ‚É,TDSE‚ð •"'l ƒV ƒ~ƒ… ƒOE•[ ƒV ƒ ‡ƒ" ‚· ‚é ‚± ‚AE ‚É ‚ae ‚Á‚ÄOE¤ ‹ † ‚³‚ê ‚Ä ‚¢ ‚é. ‚½ ‚AE ‚¦•-•" ‚Ì "d Žq ‚ðŠÜ ‚Þ OEn ‚µ ‚© Žae ‚舵 ‚¦ ‚È ‚¢ ‚AE ‚µ‚Ä ‚à,‹ß Ž-‚ª ‚ ‚« ‚à‚Ì ‚Ì-• ˜_ OE¤ ‹ † ‚É‚¨‚¢‚É‚¨‚¢ ‚Ä OEµ-§ ‰ð ‚ª "¾ ‚ç‚ê ‚é ‚AE‚¢ ‚¤ ‚± ‚AE‚Ì •d-v •« ‚AE•M-Š •« ‚ÍOEv ‚è'm ‚ê ‚È ‚¢.‚» ‚à‚» ‚à,Žž ŠÔ ‚ðŠÜ ‚Þ ƒV ƒ… ƒOE•[ ƒf ƒB ƒ"ƒK •[ •û'ö Ž® ‚ð ‚» ‚Ì ‚Ü ‚ÜOEv ŽZ ‹@ ƒV ƒ~ ƒ… ƒOE•[ ƒV ƒ ‡ ƒ"‚Å ‚«‚é ‚AE‚¢ ‚¤ ‚± ‚AE ‚É•V 'N ‚È‹Á ‚«‚ð Š´‚Š´‚ ¶‚é •l ‚à'½ ‚¢ ‚Å ‚ ‚ë ‚¤.‚Ü ‚½,HHG‚Å ƒ^ •[ ƒQ ƒb ƒg‚AE ‚µ ‚Ä ‚ae ‚-p ‚¢ ‚ç‚ê ‚éŠó ƒKƒX OE´ŽqOE´Žq ‚Í'½ ‚-‚Ì "d Žq ‚ðŠÜ ‚ñ ‚Å ‚¢ ‚é ‚ª,•K ‚¢ ‚È ‚± ‚AE‚É•‚ ‹-"x •ê OE» •Û ‚Í,‚» ‚Ì ‚¤‚¿1‚ ‚¾ ‚¯ ‚ªŽÀ OEø ƒ| ƒe ƒ" ƒV ƒƒƒ‹ ‚ðŠ´‚‚ðŠ´‚ ¶‚È‚ª ‚ç‰^ "® ‚µŽc ‚è‚Ì "d Žq ‚Ì "g "® ŠÖ •" ‚Í"€ OE‹ ‚³‚ê ‚Ä ‚¢ ‚é ‚AE‚· ‚ésingle-active-electron (SAE)•` 'oe ‚Å ‚ae ‚-•à-¾ ‚Å ‚«‚邽 ‚ß,1"d ŽqOEn ‚ÌTDSE‚Å ‚à‰ž-p "Í ˆÍ ‚Í•L ‚¢.‚± ‚Ì ‚ae ‚¤‚È ƒA ƒg•b ƒp ƒ‹ ƒX ‚Ì"-• ¶ ‚AE‚»‚ê ‚ªˆø ‚«‹N ‚±‚·OE» •Û ‚Ì-• ˜_OE¤ ‹ † ‚ÌŽå-v ‚È'ª-¬-TDSEƒV ƒ~ƒ… ƒOE•[ ƒV ƒ ‡ ƒ"•[ ‚ð •Ð ‰î ‚· ‚é ‚± ‚AE‚ª-{ •e ‚Ì-Ú"I ‚Å ‚ ‚é. ‚Ü‚¸,'ae2•Í ‚Å ‚ÍTDSE‚Ì •" 'l OEv ŽZ ƒ‚ ƒf ƒ‹ ‚É ‚ ‚¢ ‚Ä •q ‚× ‚é."Á 'è ‚ÌOEv ŽZ Žè-@ ‚ð•Ú •q ‚· ‚é ‚± ‚AE ‚Í ‚³ ‚¯,ˆÙ ‚È ‚éOE¤ ‹ † ŽÒ ‚É ‚ae ‚Á ‚Ä-p ‚¢ ‚ç‚ê ‚Ä ‚¢ ‚éŽè-@ ‚Ì ƒo ƒŠƒG •[ ƒV ƒ ‡ ƒ"‚É ‚ ‚¢ ‚ÄŠT ŠÏ ‚· ‚é.'± ‚¢ ‚Ä 'ae3•Í ‚Å ‚Í ƒtƒF ƒ€ ƒg•b ƒOE•[ƒU •[ ‚É ‚ae ‚é •‚'² "g ‚â ƒA ƒg•b ƒp ƒ‹ ƒX ‚Ì"-• ¶ ‚É‚Â ‚¢ ‚Ä,‚Ü ‚½ 'ae4•Í ‚Å ‚Í ƒA ƒg•b ƒp ƒ‹ ƒX ‚ªˆø‚ªˆø ‚«‹N ‚±‚· •V Šï ‚ÈOE» •Û ‚É‚Â ‚¢ ‚Ä,•Å •V ‚Ì-• ˜_ OE¤ ‹ † ‚Ì•¬ ‰Ê ‚ð•Ð ‰î ‚· ‚é. 'ae36Šª 'ae1• † ƒA ƒg•b OE» •Û ‚Ì-• ˜_ 25

Cite

CITATION STYLE

APA

ISHIKAWA, K. L. (2008). Theory of Attosecond Phenomena. The Review of Laser Engineering, 36(1), 25–30. https://doi.org/10.2184/lsj.36.25

Register to see more suggestions

Mendeley helps you to discover research relevant for your work.

Already have an account?

Save time finding and organizing research with Mendeley

Sign up for free