double ionization
{{Short description|Rapid removal of two electrons from an atom}}
Double ionization is a process of formation of doubly charged ions when laser radiation or charged particles like electrons,{{Cite journal |last1=Berakdar |first1=J. |last2=Lahmam-Bennani |first2=A. |last3=Dal Capello |first3=C. |date=2003 |title=The electron-impact double ionization of atoms: an insight into the four-body Coulomb scattering dynamics |url=https://www.sciencedirect.com/science/article/abs/pii/S037015730200515X |journal=Physics Reports |volume=374 |issue=2 |pages=91–164 |doi=10.1016/S0370-1573(02)00515-X|bibcode=2003PhR...374...91B |url-access=subscription }} positrons{{Cite journal |last1=Simonović |first1=N. |last2=Lukić |first2=D. |last3=Grujić |first3=P. |date=2005 |title=Double ionization by positrons near threshold |url=https://iopscience.iop.org/article/10.1088/0953-4075/38/17/006 |journal=J. Phys. B |volume=38 |issue=17 |pages=3147–3161 |doi=10.1088/0953-4075/38/17/006|bibcode=2005JPhB...38.3147S |url-access=subscription }} or heavy ions{{Cite journal |last1=DuBois |first1=R.D. |last2=Santos |first2=A.C.F. |last3=Manson |first3=S.T. |date=2014 |title=Empirical formulas for direct double ionization by bare ions: 𝑍=−1 to 92 |url=https://journals.aps.org/pra/abstract/10.1103/PhysRevA.90.052721 |journal=Physical Review A |volume=90 |pages=052721 |doi=10.1103/PhysRevA.90.052721}} are exerted on neutral atoms or molecules. Double ionization is usually less probable than single-electron ionization. Two types of double ionization are distinguished: sequential and non-sequential.
Sequential double ionization
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 ion in the ground state or an excited state) followed by detachment of the second electron from the ion.
{{Cite book | last1=Delone | first1=N. B. | author2-link=Vladimir P. Krainov | last2=Krainov | first2=V. P. | title=Multiphoton Processes in Atoms | publisher=Springer | year=2000 | isbn=3540646159| author1-link=Nikolai Borisovich Delone }}, chapter 8.
{{Gallery
|title=Examples of sequential double ionization
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|File:Sequential double ionization.pdf|Sequential double ionization
|File:NSDI through the ionic ground state.pdf|Sequential double ionization via an ionic exited state
}}
Non-sequential double ionization
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 atoms, see below), etc.
The phenomenon of non-sequential double ionization was experimentally discovered by Suran and Zapesochny for alkaline earth atoms as early as 1975.{{Cite journal | last1=Suran | first1=V. V. | last2=Zapesochny | first2=I. P. | volume=1 | year = 1975 | journal = Sov. Tech. Phys. Lett. | pages = 420 | title=Observation of Sr2+ in multiple-photon ionization of strontium|issue=11}}
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 autoionizing atomic states, located between the first and second ionization potentials.
{{Cite journal | last1 = Lambropoulos | first1 = P. | last2 = Tang | first2 = X. | last3 = Agostini | first3 = P. | last4 = Petite | first4 = G. | last5 = L'Huillier | first5 = A. | title = Multiphoton spectroscopy of doubly excited, bound, and autoionizing states of strontium | doi = 10.1103/PhysRevA.38.6165 | journal = Physical Review A | volume = 38 | issue = 12 | pages = 6165–6179 | year = 1988 | pmid = 9900374|bibcode = 1988PhRvA..38.6165L }}
File:Simultaneous photo-detachment of two electrons.pdf]]
For noble gas atoms, non-sequential double ionization was first observed by L'Huillier.
{{Cite journal | last1 = l'Huillier | first1 = A. | last2 = Lompre | first2 = L. | last3 = Mainfray | first3 = G. | last4 = Manus | first4 = C. | title = Multiply Charged Ions Formed by Multiphoton Absorption Processes in the Continuum | doi = 10.1103/PhysRevLett.48.1814 | journal = Physical Review Letters | volume = 48 | issue = 26 | pages = 1814 | year = 1982 |bibcode = 1982PhRvL..48.1814L }}
{{Cite journal | last1 = l'Huillier | first1 = A. | last2 = Lompre | first2 = L. A. | last3 = Mainfray | first3 = G. | last4 = Manus | first4 = C. | title = Multiply charged ions induced by multiphoton absorption in rare gases at 0.53 μm | doi = 10.1103/PhysRevA.27.2503 | journal = Physical Review A | volume = 27 | issue = 5 | pages = 2503 | year = 1983 |bibcode = 1983PhRvA..27.2503L }}
The interest to this phenomenon grew rapidly after it was rediscovered
{{Cite journal | last1 = Walker | first1 = B. | last2 = Mevel | first2 = E. | last3 = Yang | first3 = B. | last4 = Breger | first4 = P. | last5 = Chambaret | first5 = J. | last6 = Antonetti | first6 = A. | last7 = Dimauro | first7 = L. | last8 = Agostini | first8 = P. | doi = 10.1103/PhysRevA.48.R894 | title = Double ionization in the perturbative and tunneling regimes | journal = Physical Review A | volume = 48 | issue = 2 | pages = R894–R897 | year = 1993 | pmid = 9909791|bibcode = 1993PhRvA..48..894W }}
{{Cite journal | last1 = Walker | first1 = B. | last2 = Sheehy | first2 = B. | last3 = Dimauro | first3 = L. | last4 = Agostini | first4 = P. | last5 = Schafer | first5 = K. | last6 = Kulander | first6 = K. | doi = 10.1103/PhysRevLett.73.1227 | title = Precision Measurement of Strong Field Double Ionization of Helium | journal = Physical Review Letters | volume = 73 | issue = 9 | pages = 1227–1230 | year = 1994 | pmid = 10057657|bibcode = 1994PhRvL..73.1227W }}
in infrared fields and for higher intensities. Multiple ionization has also been observed.
{{Cite journal | last1 = Rudenko | first1 = A. | last2 = Zrost | first2 = K. | last3 = Feuerstein | first3 = B. | last4 = De Jesus | first4 = V. | last5 = Schröter | first5 = C. | last6 = Moshammer | first6 = R. | last7 = Ullrich | first7 = J. | title = Correlated Multielectron Dynamics in Ultrafast Laser Pulse Interactions with Atoms | doi = 10.1103/PhysRevLett.93.253001 | journal = Physical Review Letters | volume = 93 | issue = 25 | year = 2004 | pmid = 15697894|arxiv = physics/0408065 |bibcode = 2004PhRvL..93y3001R | page=253001| s2cid = 40450686 }}
{{Cite journal | last1 = Zrost | first1 = K. | last2 = Rudenko | first2 = A. | last3 = Ergler | first3 = T. | last4 = Feuerstein | first4 = B. | last5 = Jesus | first5 = V. L. B. D. | last6 = Schröter | first6 = C. D. | last7 = Moshammer | first7 = R. | last8 = Ullrich | first8 = J. | doi = 10.1088/0953-4075/39/13/S10 | title = Multiple ionization of Ne and Ar by intense 25 fs laser pulses: Few-electron dynamics studied with ion momentum spectroscopy | journal = Journal of Physics B: Atomic, Molecular and Optical Physics | volume = 39 | issue = 13 | pages = S371 | year = 2006 |bibcode = 2006JPhB...39S.371Z | s2cid = 122414336 }}
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
{{Cite journal | last1 = Corkum | first1 = P. | title = Plasma perspective on strong field multiphoton ionization | doi = 10.1103/PhysRevLett.71.1994 | journal = Physical Review Letters | volume = 71 | issue = 13 | pages = 1994–1997 | year = 1993 | pmid = 10054556|bibcode = 1993PhRvL..71.1994C | s2cid = 29947935 | url = https://nrc-publications.canada.ca/eng/view/accepted/?id=c16dde3a-0d05-4437-bca6-3292fdd9d9ff }}
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 high harmonic generation.
Dynamics of double ionization within the three-step model strongly depends on the laser field intensity. The maximum energy (in atomic units) gained by the recolliding electron from the laser field is , where
is the ponderomotive energy, is the laser field strength, and is the laser frequency. Even when is far below ionization potential experiments have observed correlated ionization.
{{Cite journal | last1 = Zeidler | first1 = D. | last2 = Staudte | first2 = A. | last3 = Bardon | first3 = A. B. | last4 = Villeneuve | first4 = D. M. | last5 = Dörner | first5 = R. | last6 = Corkum | first6 = P. B. | doi = 10.1103/PhysRevLett.95.203003 | title = Controlling Attosecond Double Ionization Dynamics via Molecular Alignment | journal = Physical Review Letters | volume = 95 | issue = 20 | year = 2005 | pmid = 16384053|bibcode = 2005PhRvL..95t3003Z | page=203003| url = https://nrc-publications.canada.ca/eng/view/accepted/?id=8ca16c24-5317-4a60-80fc-b6e55f674b9f }}
{{Cite journal | last1 = Weckenbrock | first1 = M. | last2 = Zeidler | first2 = D. | last3 = Staudte | first3 = A. | last4 = Weber | first4 = T. | last5 = Schöffler | first5 = M. | last6 = Meckel | first6 = M. | last7 = Kammer | first7 = S. | last8 = Smolarski | first8 = M. | last9 = Jagutzki | first9 = O. | last10 = Bhardwaj | first10 = V. | last11 = Rayner | first11 = D. | last12 = Villeneuve | first12 = D. | last13 = Corkum | first13 = P. | last14 = Dörner | first14 = R. | title = Fully Differential Rates for Femtosecond Multiphoton Double Ionization of Neon | doi = 10.1103/PhysRevLett.92.213002 | journal = Physical Review Letters | volume = 92 | issue = 21 | year = 2004 | pmid = 15245277|bibcode = 2004PhRvL..92u3002W | page=213002| url = https://nrc-publications.canada.ca/eng/view/accepted/?id=b728bd1f-4973-4371-934c-fa42311be1e8 }}
{{Cite journal | last1 = Liu | first1 = Y. | last2 = Tschuch | first2 = S. | last3 = Rudenko | first3 = A. | last4 = Dürr | first4 = M. | last5 = Siegel | first5 = M. | last6 = Morgner | first6 = U. | last7 = Moshammer | first7 = R. | last8 = Ullrich | first8 = J. | doi = 10.1103/PhysRevLett.101.053001 | title = Strong-Field Double Ionization of Ar below the Recollision Threshold | journal = Physical Review Letters | volume = 101 | issue = 5 | pages = 053001 | year = 2008 | pmid = 18764387|bibcode = 2008PhRvL.101e3001L | url = http://www.repo.uni-hannover.de/handle/123456789/3326 }}
As opposed to the high- regime ()
{{Cite journal | last1 = Yudin | first1 = G. | last2 = Ivanov | first2 = M. | doi = 10.1103/PhysRevA.63.033404 | title = Physics of correlated double ionization of atoms in intense laser fields: Quasistatic tunneling limit | journal = Physical Review A | volume = 63 | issue = 3 | pages = 033404 | year = 2001 |bibcode = 2001PhRvA..63c3404Y | url = https://nrc-publications.canada.ca/eng/view/accepted/?id=7a64c29b-0090-4152-9f57-034a305a9246 }}
{{Cite journal | last1 = Becker | first1 = A. | last2 = Faisal | first2 = F. H. M. | s2cid = 14675241 | doi = 10.1088/0953-4075/38/3/R01 | title = Intense-field many-body S-matrix theory | journal = Journal of Physics B: Atomic, Molecular and Optical Physics | volume = 38 | issue = 3 | pages = R1 | year = 2005 |bibcode = 2005JPhB...38R...1B }}
{{Cite journal | last1 = Staudte | first1 = A. | last2 = Ruiz | first2 = C. | last3 = Schöffler | first3 = M. | last4 = Schössler | first4 = S. | last5 = Zeidler | first5 = D. | last6 = Weber | first6 = T. | last7 = Meckel | first7 = M. | last8 = Villeneuve | first8 = D. | last9 = Corkum | first9 = P. | last10 = Becker | first10 = A. | last11 = Dörner | first11 = R. | title = Binary and Recoil Collisions in Strong Field Double Ionization of Helium | doi = 10.1103/PhysRevLett.99.263002 | journal = Physical Review Letters | volume = 99 | issue = 26 | pages = 263002 | year = 2007 | pmid = 18233574|bibcode = 2007PhRvL..99z3002S | url = https://nrc-publications.canada.ca/eng/view/accepted/?id=77cdbaab-c33b-4925-881e-5c68e1054226 }}
{{Cite journal | last1 = Rudenko | first1 = A. | last2 = De Jesus | first2 = V. | last3 = Ergler | first3 = T. | last4 = Zrost | first4 = K. | last5 = Feuerstein | first5 = B. | last6 = Schröter | first6 = C. | last7 = Moshammer | first7 = R. | last8 = Ullrich | first8 = J. | doi = 10.1103/PhysRevLett.99.263003 | title = Correlated Two-Electron Momentum Spectra for Strong-Field Nonsequential Double Ionization of He at 800 nm | journal = Physical Review Letters | volume = 99 | issue = 26 | year = 2007 | pmid = 18233575|bibcode = 2007PhRvL..99z3003R | page=263003}}
in the low- regime () the assistance of the laser field during the
recollision is vital.
Classical and quantum analysis
{{Cite journal | last1 = Haan | first1 = S. | last2 = Breen | first2 = L. | last3 = Karim | first3 = A. | last4 = Eberly | first4 = J. | title = Variable Time Lag and Backward Ejection in Full-Dimensional Analysis of Strong-Field Double Ionization | doi = 10.1103/PhysRevLett.97.103008 | journal = Physical Review Letters | volume = 97 | issue = 10 | year = 2006 | pmid = 17025816|bibcode = 2006PhRvL..97j3008H | page=103008}}
{{Cite journal | last1 = Ho | first1 = P. | last2 = Eberly | first2 = J. | doi = 10.1103/PhysRevLett.97.083001 | title = In-Plane Theory of Nonsequential Triple Ionization | journal = Physical Review Letters | volume = 97 | issue = 8 | year = 2006 | pmid = 17026298|arxiv = physics/0605026 |bibcode = 2006PhRvL..97h3001H | page=083001| s2cid = 8978621 }}
{{Cite journal | last1 = Figueira De Morisson Faria | first1 = C. | last2 = Liu | first2 = X. | last3 = Becker | first3 = W. | title = Classical aspects of laser-induced non-sequential double ionization above and below the threshold | doi = 10.1080/09500340500227869 | journal = Journal of Modern Optics | volume = 53 | issue = 1–2 | pages = 193–206 | year = 2006 |bibcode = 2006JMOp...53..193F | s2cid = 120011073 }}
of the low- 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 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.
{{Cite journal | last1 = Bondar | first1 = D. | last2 = Liu | first2 = W. K. | last3 = Ivanov | first3 = M. | title = Two-electron ionization in strong laser fields below intensity threshold: Signatures of attosecond timing in correlated spectra | doi = 10.1103/PhysRevA.79.023417 | journal = Physical Review A | volume = 79 | issue = 2 | pages = 023417 | year = 2009 |arxiv = 0809.2630 |bibcode = 2009PhRvA..79b3417B | s2cid = 119275628 }}
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
{{Gallery
|title=Non-sequential double ionization of noble gas atoms
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|File:NSDI in high-Up regime.pdf|The high- regime
|File:NSDI in low-Up regime.pdf|The low- regime
}}
See also
- List of laser articles
- Nonlinear optics
- Photoionization
- Ionization
- High harmonic generation
- Above threshold ionization
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