Transient
Superconductivity in optically modulated YBa2Cu3O6+x
Stefan Kaiser
Max‐Planck Institut
für Struktur und Dynamik der Materie,
Center for Free Electron Laser Science,
Photo‐stimulation with
femtosecond mid‐infrared pulses allows us to induce a
non‐equilibrium superconducting state in YBa2Cu3O6+x at
temperatures as high
as
300 K. Its transient response is probed via THz time‐domain
spectroscopy.
The parent, undoped compounds of high‐Tc cuprates are antiferromagnetic
Mott
insulators, whose physical properties are strongly modified
upon doping the Cu‐
O planes with a few percent charge carriers. One
region of their phase diagram
which has attracted much attention is the so‐called pseudogap phase [1,2], found
below a characteristic temperature T* in moderately‐doped
materials. The origin
of
this gapped, but non‐superconducting state has been attributed to a
variety of
microscopic phenomena, ranging from a precursor
superconducting state with
pre‐formed Cooper pairs without phase coherence, to a
scenario where
electronic correlations compete with superconductivity.
So far, only optical excitation in the visible or
near infrared has been performed
on
high‐Tc cuprates
[3‐5]. Such experiments have investigated the
relaxation of
hot incoherent quasiparticles back into the Cooper‐pair
condensate. Therefore,
superconductivity could not be triggered directly by the light
field.
By making use of mid‐infrared pulses,
phase transitions have been photoinduced
in
strongly‐correlated electron systems through resonant
excitation of lattice
vibrational modes [6]. In particular, we have shown that light
can induce
superconductivity in La1.675Eu0.2Sr0.125CuO4 at temperatures as high
as 20 K, by
melting the competing spin‐ and charge‐order in the so‐called
stripe phase [7].
Here, we set out to establish phase coherence in YBa2Cu3O6+x
for temperatures
far above Tc. Therefore high intensity optical
pulses at THz frequencies are used
to
dynamically modulate the crystallographic structure. This creates a high
mobility state for base temperatures far above Tc, as evidenced by the
appearance of a plasma edge in the c‐axis
reflectivity and a divergent imaginary
optical conductivity at low frequencies. We identify this state as an
inhomogeneous transient superconductor, which for low doping is
observed
even as high as room temperature [8]. Using ultra‐broadband
THz pulses we are
able to investigate the redistribution of interlayer coherence within the bi‐layer
structure of YBCO [9]. Ultrafast x‐ray
experiments at LCLS allow us observing the
nonlinear phonon dynamics after the lattice excitation and
to reconstruct the
crystal structure in the transient superconducting state [10].
[1] T. Timusk and B. Statt, "The pseudogap in
high‐Tc SC:
an experimental survey," Rep. Prog. Phys. 62, 61 (1999).
[2] D. N. Basov and T. Timusk,
"Electrodynamics of high‐Tc superconductors,"
Rev. Mod. Phys. 77, 721 (2005).
[3] J. Demsar, B. Podobnik, V. V. Kabanov, et
al., "Superconducting Gap Δc,
the Pseudogap Δp,
and pair fluctuations above
Tc in
overdoped Y1‐xCaxBa2Cu3O7‐δ from
Femtosecond Time‐Domain Spectroscopy," Phys. Rev. Lett. 82, 4198 (1999).
[4] R. A. Kaindl, , et al. "Ultrafast Mid‐Infrared
Response of YBa2Cu3O7‐δ," Science 287, 470 (2000).
[5] R. D. Averitt, G.
Rodriguez, A. I. Lobad, et al., "Nonequilibrium superconductivity and quasiparticle dynamics
in
YBa2Cu3O7‐δ," Phys.
Rev. B 63, 140502 (2001).
[6] M. Rini, R. I. Tobey, N. Dean, et al. "Control of the
electronic phase of a manganite by mode‐selective
vibrational
excitation," Nature 449, 72‐74
(2007).
[7] D. Fausti, R. I. Tobey, N. Dean. S. Kaiser, A. Dienst,
M. C. Hoffmann,
"Light‐Induced
Superconductivity in a Stripe‐Ordered Cuprate,"
Science 331, 189 (2011).
[8] S. Kaiser, D. Nicoletti,
C. R. Hunt, W. Hu, I. Gierz,
H. Y. Liu, M. Le Tacon, T. Loew,
D. Haug, B. Keimer, A. Cavalleri,
“Light‐induced
inhomogeneous superconductivity far above Tc in YBa2Cu3O6+x”
arXiv:1205.4661 (2013)
[9] W. Hu, I. Gierz, D. Nicoletti, S. Kaiser,
C. R. Hunt, et al. “Enhancement of superconductivity by
redistribution of
interlayer coupling in optically stimulated YBa2Cu3O6.5”,
arXiv1308.3204 (2013).
[10] R. Mankowsky, M. Forst et al. (unpublished) .
Host: Prof. E. Andrei