Attosecond transient absorption probing of electronic superpositions of bound states in neon: detection of quantum beats

Electronic wavepackets composed of multiple bound excited states of atomic neon lying between 19.6 and 21.5 eV are launched using an isolated attosecond pulse. Individual quantum beats of the wavepacket are detected by perturbing the induced polarization of the medium with a time-delayed few-femtosecond near-infrared (NIR) pulse via coupling the individual states to multiple neighboring levels. All of the initially excited states are monitored simultaneously in the attosecond transient absorption spectrum, revealing Lorentzian to Fano lineshape spectral changes as well as quantum beats. The most prominent beating of the several that were observed was in the spin–orbit split 3d absorption features, which has a 40 femtosecond period that corresponds to the spin–orbit splitting of 0.1 eV. The few-level models and multilevel calculations confirm that the observed magnitude of oscillation depends strongly on the spectral bandwidth and tuning of the NIR pulse and on the location of possible coupling states.

[1]  J. Campos,et al.  Experimental absolute transition probabilities of lines from the 3d′(3/2) 2 level of Ne i , 1977 .

[2]  O. Misochko Nonclassical states of lattice excitations: squeezed and entangled phonons , 2013 .

[3]  S. Leone,et al.  Intensity dependence of light-induced states in transient absorption of laser-dressed helium measured with isolated attosecond pulses , 2013 .

[4]  S. Leone,et al.  Alternating absorption features during attosecond-pulse propagation in a laser-controlled gaseous medium , 2013 .

[5]  R. Mathies,et al.  Analysis of femtosecond dynamic absorption spectra of nonstationary states. , 1992, Annual review of physical chemistry.

[6]  Z. Chang,et al.  Double optical gating of high-order harmonic generation with carrier-envelope phase stabilized lasers. , 2008, Physical review letters.

[7]  B. L. Henke,et al.  X-Ray Interactions: Photoabsorption, Scattering, Transmission, and Reflection at E = 50-30,000 eV, Z = 1-92 , 1993 .

[8]  C. Keitel,et al.  Lorentz Meets Fano in Spectral Line Shapes: A Universal Phase and Its Laser Control , 2013, Science.

[9]  S. Leone,et al.  High-spectral-resolution attosecond absorption spectroscopy of autoionization in xenon , 2014 .

[10]  S. Leone,et al.  Light-induced states in attosecond transient absorption spectra of laser-dressed helium , 2012 .

[11]  J. Campos,et al.  Transition probabilities of lines with origin in the 3d'(5/2)2, 3d'(5/2)3 and 3d'(3/2)1 levels of Ne(I). , 1978 .

[12]  J. Campos,et al.  Transition probabilities of some lines of Ne(I) , 1979 .

[13]  V. Yakovlev,et al.  Modelling attosecond probing of electron wavepacket dynamics in non-aligned molecules , 2008 .

[14]  M. Seaton OSCILLATOR STRENGTHS IN NE I , 1998 .

[15]  Zenghu Chang,et al.  Subcycle laser control and quantum interferences in attosecond photoabsorption of neon , 2013 .

[16]  A. Wirsing,et al.  Control of coherent excitation of neon in the extreme ultraviolet regime. , 2011, Faraday discussions.

[17]  Feng He,et al.  Attosecond time-resolved autoionization of argon. , 2010, Physical review letters.

[18]  Application of a numerical-basis-state method to strong-field excitation and ionization of hydrogen atoms , 2012 .

[19]  Yi Wu,et al.  Sub-cycle Oscillations in Virtual States Brought to Light , 2013, Scientific Reports.

[20]  J. Gordon,et al.  Dynamics of spectral hole burning , 1988 .

[21]  M. Abel,et al.  Time-resolved spectroscopy of attosecond quantum dynamics , 2008 .

[22]  Henrik Stapelfeldt,et al.  Colloquium: Aligning molecules with strong laser pulses , 2003 .

[23]  Lindberg,et al.  Transient oscillations and dynamic Stark effect in semiconductors. , 1988, Physical review. B, Condensed matter.

[24]  M. Vrakking,et al.  Experimental observation of revival structures in picosecond laser-induced alignment of I2. , 2001, Physical review letters.

[25]  C. Fischer,et al.  Breit–Pauli energy levels, lifetimes, and transition probabilities for the beryllium-like to neon-like sequences☆ , 2004 .

[26]  A. Baclawski Experimental transition probabilities and J-file sum rule test for the transition array 3p–3d in neutral neon , 2008 .

[27]  I. A. Walmsley,et al.  Self-referencing spectral interferometry for measuring ultrashort optical pulses , 1999 .

[28]  Ahmed H. Zewail,et al.  Femtochemistry: Atomic-Scale Dynamics of the Chemical Bond† , 2000 .

[29]  K. Schafer,et al.  Laser-imposed phase in resonant absorption of an isolated attosecond pulse , 2013 .

[30]  Kenneth J. Schafer,et al.  Transient absorption and reshaping of ultrafast XUV light by laser-dressed helium , 2010, 1010.4558.

[31]  Man Mohan,et al.  Energies, Oscillator Strengths, and Lifetimes for Neon-like Ions Up to Kr XXVII , 1993 .

[32]  Stephen R. Leone,et al.  Real-time observation of valence electron motion , 2010, Nature.

[33]  M. Abel,et al.  Tunable frequency-controlled isolated attosecond pulses characterized by either 750 nm or 400 nm wavelength streak fields. , 2010, Optics express.