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Double ionization

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131:.  The interest to this phenomenon grew rapidly after it was rediscovered in infrared fields and for higher intensities. Multiple ionization has also been observed.  The mechanism of non-sequential double ionization in noble gas atoms differs from the one in alkaline earth atoms. For noble gas atoms in infrared laser fields, following one-electron ionization, the liberated electron can recollide with the parent ion. This electron acts as an "atomic antenna", absorbing the energy from the laser field between ionization and recollision and depositing it into the parent ion. Inelastic scattering on the parent ion results in further collisional excitation and/or ionization. This mechanism is known as the three-step model of non-sequential double ionization, which is also closely related to the three step model of 647: 509:
order of the quarter-cycle of the driving field. In these two cases, the electrons appear in different quadrants of the correlated spectrum. If following the recollision, the electrons are ejected nearly simultaneously, their parallel momenta have equal signs, and both electrons are driven by the laser field in the same direction toward the detector . If after the recollision, the electrons are ejected with a substantial delay (quarter-cycle or more), they end up going in the opposite directions. These two types of dynamics produce distinctly different correlated spectra (compare experimental results with .
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Non-sequential double ionization is a process whose mechanism differs (in any detail) from the sequential one. For example, both the electrons leave the system simultaneously (as in alkaline earth atoms, see below), the second electron's liberation is assisted by the first electron (as in noble gas
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regime demonstrates the following two ways of electron ejection after the recollision: First, the two electrons can be freed with little time delay compared to the quarter-cycle of the driving laser field. Second, the time delay between the ejection of the first and the second electron is of the
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Zrost, K.; Rudenko, A.; Ergler, T.; Feuerstein, B.; Jesus, V. L. B. D.; Schröter, C. D.; Moshammer, R.; Ullrich, J. (2006). "Multiple ionization of Ne and Ar by intense 25 fs laser pulses: Few-electron dynamics studied with ion momentum spectroscopy".
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as early as 1975. Despite extensive studies, the details of double ionization in alkaline earth atoms remain unknown. It is supposed that double ionization in this case is realized by transitions of both the electrons through the spectrum of
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Rudenko, A.; De Jesus, V.; Ergler, T.; Zrost, K.; Feuerstein, B.; Schröter, C.; Moshammer, R.; Ullrich, J. (2007). "Correlated Two-Electron Momentum Spectra for Strong-Field Nonsequential Double Ionization of He at 800 nm".
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Sequential double ionization is a process of formation of doubly charged ions consisting of two single-electron ionization events: the first electron is removed from a neutral atom/molecule (leaving a singly charged
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Liontos, I.; Bolovinos, A.; Cohen, S.; Lyras, A. (2004). "Single and double ionization of magnesium via four-photon excitation of the 3p^{2}^{1}S_{0} autoionizing state: Experimental and theoretical analysis".
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Weckenbrock, M.; Zeidler, D.; Staudte, A.; Weber, T.; Schöffler, M.; Meckel, M.; Kammer, S.; Smolarski, M.; Jagutzki, O.; Bhardwaj, V.; Rayner, D.; Villeneuve, D.; Corkum, P.; Dörner, R. (2004).
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Rudenko, A.; Zrost, K.; Feuerstein, B.; De Jesus, V.; Schröter, C.; Moshammer, R.; Ullrich, J. (2004). "Correlated Multielectron Dynamics in Ultrafast Laser Pulse Interactions with Atoms".
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Bondar, I. I.; Suran, V. V.; Dudich, M. I. (2000). "Resonant structure in doubly charged ion formation during multiphoton ionization of Sr and Ba atoms by infrared laser radiation".
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Bondar, D.; Liu, W. K.; Ivanov, M. (2009). "Two-electron ionization in strong laser fields below intensity threshold: Signatures of attosecond timing in correlated spectra".
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Walker, B.; Mevel, E.; Yang, B.; Breger, P.; Chambaret, J.; Antonetti, A.; Dimauro, L.; Agostini, P. (1993). "Double ionization in the perturbative and tunneling regimes".
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Lambropoulos, P.; Tang, X.; Agostini, P.; Petite, G.; L'Huillier, A. (1988). "Multiphoton spectroscopy of doubly excited, bound, and autoionizing states of strontium".
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Figueira De Morisson Faria, C.; Liu, X.; Becker, W. (2006). "Classical aspects of laser-induced non-sequential double ionization above and below the threshold".
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is a process of formation of doubly charged ions when laser radiation is exerted on neutral atoms or molecules. Double ionization is usually less probable than
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Haan, S.; Breen, L.; Karim, A.; Eberly, J. (2006). "Variable Time Lag and Backward Ejection in Full-Dimensional Analysis of Strong-Field Double Ionization".
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Walker, B.; Sheehy, B.; Dimauro, L.; Agostini, P.; Schafer, K.; Kulander, K. (1994). "Precision Measurement of Strong Field Double Ionization of Helium".
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Staudte, A.; Ruiz, C.; Schöffler, M.; Schössler, S.; Zeidler, D.; Weber, T.; Meckel, M.; Villeneuve, D.; Corkum, P.; Becker, A.; Dörner, R. (2007).
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l'Huillier, A.; Lompre, L. A.; Mainfray, G.; Manus, C. (1983). "Multiply charged ions induced by multiphoton absorption in rare gases at 0.53 ÎĽm".
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l'Huillier, A.; Lompre, L.; Mainfray, G.; Manus, C. (1982). "Multiply Charged Ions Formed by Multiphoton Absorption Processes in the Continuum".
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Bondar’, I. I.; Suran, V. V. (1998). "Resonance structure of doubly-charged-ion production during laser dielectronic ionization of atoms".
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Dynamics of double ionization within the three-step model strongly depends on the laser field intensity. The maximum energy (in
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The phenomenon of non-sequential double ionization was experimentally discovered by Suran and Zapesochny for
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Liu, Y.; Tschuch, S.; Rudenko, A.; DĂĽrr, M.; Siegel, M.; Morgner, U.; Moshammer, R.; Ullrich, J. (2008).
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Suran, V. V.; Zapesochny, I. P. (1975). "Observation of Sr in multiple-photon ionization of strontium".
1494:"Physics of correlated double ionization of atoms in intense laser fields: Quasistatic tunneling limit" 438: 368: 1837: 1784: 1733: 1680: 1637: 1590: 1540: 1505: 1458: 1408: 1358: 1324: 1266: 1216: 1159: 1101: 1058: 1023: 988: 945: 906: 862: 819: 788: 777:"The two-electron mechanism of Ba ion formation in the ionization of Ba atoms by YAG-laser radiation" 741: 309: 235: 117: 106: 97: 684: 145: 1853: 1827: 1800: 1757: 1723: 1556: 1290: 1232: 1183: 1149: 961: 878: 835: 128: 1749: 1696: 1653: 1606: 1474: 1424: 1374: 1345:
Zeidler, D.; Staudte, A.; Bardon, A. B.; Villeneuve, D. M.; Dörner, R.; Corkum, P. B. (2005).
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Ho, P.; Eberly, J. (2006). "In-Plane Theory of Nonsequential Triple Ionization".
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Becker, A.; Faisal, F. H. M. (2005). "Intense-field many-body S-matrix theory".
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experiments have observed correlated ionization.  As opposed to the high-
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atoms, non-sequential double ionization was first observed by
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Journal of Physics B: Atomic, Molecular and Optical Physics
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Journal of Physics B: Atomic, Molecular and Optical Physics
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Journal of Physics B: Atomic, Molecular and Optical Physics
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Journal of Physics B: Atomic, Molecular and Optical Physics
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Journal of Experimental and Theoretical Physics Letters
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Sequential double ionization via an ionic exited state
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atomic states, located between the first and second
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Even when 14: 471:{\displaystyle 3.2U_{p}<I_{p}} 401:{\displaystyle 3.2U_{p}>I_{p}} 258:is the laser field strength, and 656: 645: 565: 526: 88:Non-sequential double ionization 72: 60: 1492:Yudin, G.; Ivanov, M. (2001). 1471:10.1103/PhysRevLett.101.053001 689:Multiphoton Processes in Atoms 1: 1746:10.1103/PhysRevLett.97.083001 1693:10.1103/PhysRevLett.97.103008 1650:10.1103/PhysRevLett.99.263003 1603:10.1103/PhysRevLett.99.263002 1421:10.1103/PhysRevLett.92.213002 1371:10.1103/PhysRevLett.95.203003 1172:10.1103/PhysRevLett.93.253001 958:10.1088/0953-4075/43/9/095602 168:{\displaystyle \sim 3.2U_{p}} 67:Sequential double ionization 30:Sequential double ionization 1279:10.1103/PhysRevLett.71.1994 1229:10.1088/0953-4075/39/13/S10 1114:10.1103/PhysRevLett.73.1227 1001:10.1103/PhysRevLett.48.1814 875:10.1088/0953-4075/33/20/304 1903: 1850:10.1103/PhysRevA.79.023417 1553:10.1088/0953-4075/38/3/R01 1518:10.1103/PhysRevA.63.033404 919:10.1103/PhysRevA.70.033403 639:Above threshold ionization 24:single-electron ionization 1797:10.1080/09500340500227869 1777:Journal of Modern Optics 1071:10.1103/PhysRevA.48.R894 1036:10.1103/PhysRevA.27.2503 754:10.1103/PhysRevA.38.6165 634:High harmonic generation 301:{\displaystyle 3.2U_{p}} 133:high harmonic generation 93:atoms, see below), etc. 1716:Physical Review Letters 1673:Physical Review Letters 1630:Physical Review Letters 1583:Physical Review Letters 1451:Physical Review Letters 1401:Physical Review Letters 1351:Physical Review Letters 1311:Kuchiev, M. Y. (1987). 1259:Physical Review Letters 1142:Physical Review Letters 1094:Physical Review Letters 981:Physical Review Letters 271:{\displaystyle \omega } 614:List of laser articles 593: 554: 502: 472: 429: 402: 359: 332: 302: 272: 252: 228: 169: 120: 799:on December 21, 2012. 715:Sov. Tech. Phys. Lett 594: 592:{\displaystyle U_{p}} 555: 553:{\displaystyle U_{p}} 503: 501:{\displaystyle U_{p}} 473: 430: 428:{\displaystyle U_{p}} 403: 360: 358:{\displaystyle U_{p}} 333: 331:{\displaystyle I_{p}} 303: 273: 253: 229: 170: 115: 107:ionization potentials 576: 537: 485: 439: 412: 369: 342: 315: 310:ionization potential 282: 262: 242: 236:ponderomotive energy 179: 146: 118:alkaline earth atoms 98:alkaline earth atoms 1842:2009PhRvA..79b3417B 1789:2006JMOp...53..193F 1738:2006PhRvL..97h3001H 1685:2006PhRvL..97j3008H 1642:2007PhRvL..99z3003R 1595:2007PhRvL..99z3002S 1545:2005JPhB...38R...1B 1510:2001PhRvA..63c3404Y 1463:2008PhRvL.101e3001L 1413:2004PhRvL..92u3002W 1363:2005PhRvL..95t3003Z 1329:1987JETPL..45..404K 1271:1993PhRvL..71.1994C 1253:Corkum, P. (1993). 1221:2006JPhB...39S.371Z 1164:2004PhRvL..93y3001R 1106:1994PhRvL..73.1227W 1063:1993PhRvA..48..894W 1028:1983PhRvA..27.2503L 993:1982PhRvL..48.1814L 950:2010JPhB...43i5602L 911:2004PhRvA..70c3403L 867:2000JPhB...33.4243B 824:1998JETPL..68..837B 793:1993JETP...76..381B 746:1988PhRvA..38.6165L 663:Science portal 652:Physics portal 589: 550: 498: 468: 425: 398: 355: 328: 298: 268: 248: 224: 165: 121: 1882:Quantum mechanics 1820:Physical Review A 1498:Physical Review A 1265:(13): 1994–1997. 1051:Physical Review A 1016:Physical Review A 899:Physical Review A 740:(12): 6165–6179. 734:Physical Review A 251:{\displaystyle F} 222: 20:Double ionization 1894: 1887:Nonlinear optics 1862: 1861: 1835: 1815: 1809: 1808: 1783:(1–2): 193–206. 1772: 1766: 1765: 1731: 1711: 1705: 1704: 1668: 1662: 1661: 1624: 1615: 1614: 1574: 1565: 1564: 1528: 1522: 1521: 1489: 1483: 1482: 1442: 1433: 1432: 1392: 1383: 1382: 1342: 1333: 1332: 1313:"Atomic Antenna" 1308: 1299: 1298: 1250: 1241: 1240: 1203: 1192: 1191: 1157: 1137: 1126: 1125: 1100:(9): 1227–1230. 1089: 1083: 1082: 1057:(2): R894–R897. 1046: 1040: 1039: 1011: 1005: 1004: 976: 970: 969: 929: 923: 922: 893: 887: 886: 850: 844: 843: 832:10.1134/1.567802 807: 801: 800: 795:. Archived from 772: 766: 765: 729: 723: 722: 710: 704: 702: 677: 661: 660: 650: 649: 619:Nonlinear optics 598: 596: 595: 590: 588: 587: 569: 559: 557: 556: 551: 549: 548: 530: 507: 505: 504: 499: 497: 496: 477: 475: 474: 469: 467: 466: 454: 453: 434: 432: 431: 426: 424: 423: 407: 405: 404: 399: 397: 396: 384: 383: 364: 362: 361: 356: 354: 353: 337: 335: 334: 329: 327: 326: 307: 305: 304: 299: 297: 296: 277: 275: 274: 269: 257: 255: 254: 249: 233: 231: 230: 225: 223: 221: 220: 219: 206: 205: 196: 191: 190: 174: 172: 171: 166: 164: 163: 76: 64: 1902: 1901: 1897: 1896: 1895: 1893: 1892: 1891: 1867: 1866: 1865: 1817: 1816: 1812: 1774: 1773: 1769: 1729:physics/0605026 1713: 1712: 1708: 1670: 1669: 1665: 1626: 1625: 1618: 1576: 1575: 1568: 1530: 1529: 1525: 1491: 1490: 1486: 1444: 1443: 1436: 1394: 1393: 1386: 1344: 1343: 1336: 1310: 1309: 1302: 1252: 1251: 1244: 1205: 1204: 1195: 1155:physics/0408065 1139: 1138: 1129: 1091: 1090: 1086: 1048: 1047: 1043: 1013: 1012: 1008: 978: 977: 973: 931: 930: 926: 895: 894: 890: 852: 851: 847: 809: 808: 804: 774: 773: 769: 731: 730: 726: 712: 711: 707: 699: 679: 678: 674: 670: 655: 654: 644: 624:Photoionization 610: 605: 604: 603: 600: 579: 574: 573: 570: 561: 540: 535: 534: 531: 520: 519: 488: 483: 482: 458: 445: 437: 436: 415: 410: 409: 388: 375: 367: 366: 345: 340: 339: 318: 313: 312: 288: 280: 279: 260: 259: 240: 239: 211: 207: 197: 182: 177: 176: 155: 144: 143: 90: 85: 84: 83: 80: 77: 68: 65: 54: 53: 32: 17: 12: 11: 5: 1900: 1898: 1890: 1889: 1884: 1879: 1869: 1868: 1864: 1863: 1810: 1767: 1706: 1679:(10): 103008. 1663: 1636:(26): 263003. 1616: 1589:(26): 263002. 1566: 1523: 1484: 1434: 1407:(21): 213002. 1384: 1357:(20): 203003. 1334: 1300: 1242: 1193: 1148:(25): 253001. 1127: 1084: 1041: 1006: 971: 924: 888: 845: 802: 767: 724: 705: 697: 685:Krainov, V. 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Index

single-electron ionization
ion
ground state
excited state
Sequential double ionization
Sequential double ionization via an ionic exited state
alkaline earth atoms
autoionizing
ionization potentials

alkaline earth atoms
noble gas
L'Huillier
high harmonic generation
atomic units
ponderomotive energy
ionization potential
noble gas
The high-'"`UNIQ--postMath-0000000C-QINU`"' regime
The low-'"`UNIQ--postMath-0000000D-QINU`"' regime
List of laser articles
Nonlinear optics
Photoionization
Ionization
High harmonic generation
Above threshold ionization
icon
Physics portal
icon
Science portal

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