Title: Coherent Raman spectroscopy of Cd1xMnxTe quantum wells
1Coherent Raman spectroscopy ofCd1-xMnxTe quantum
wells
- Lowenna Smith, Daniel Wolverson,
- Stephen Bingham and J. John Davies
- Department of Physics,
- University of Bath, Bath, UK
M. Lentze and J. Geurts Physikalisiches Institut,
EP III, Universität Würzburg, Am Hubland, 97074
Würzburg, Germany M. Wiater, G. Karczewski,
and T. Wojtowicz Institute of Physics, Polish
Academy of Sciences, Warsaw, Poland
2Plan
- Spin Flip Raman Scattering (SFRS)
- Coherent Raman (CRESR)
- Mn2 in Cd1-xMnxTe quantum wells
3Spin flip Raman scattering
- Sample excited by laser in resonance with
excitonic intermediate state - When a magnetic field is applied, weak sidebands
at the Zeeman splitting appear on either side of
the laser line - k.p theory predicts g-factors of band carriers
- carriers at point defects must be modelled by
spin Hamiltonians relevant to their symmetry
4Spin flip Raman of Cd1-xMnxTe QWs
- Spin flip Raman scattering occurs between the
S5/2 Mn2 3d5 levels with Dms1 - Resonance is again via an excitonic intermediate
state - Many multiples of the fundamental Dms1 signal
are seen.
...
Stühler et al, PRB 49 (1994) 7345 PRL 74 (1995)
2567 Koenig et al, PRB 61 (2000),16870
5What is coherent Raman ESR?
- ESR can provide higher resolution than SFRS...
- but ESR does not have the selectivity of SFRS (no
excitonic resonance) - ESR also doesnt have the sensitivity of optical
techniques
Electron Spin Resonance
Coherent Raman ESR
- Coherent Raman-detected ESR (CRESR) has both.
6How does CRESR work?
- Laser beam reflects from (or passes through)
sample and induces coherence between ground state
1gt and the intermediate excitonic state 3gt - At spin resonance field, microwaves induce
coherence between the spin states 1gt and 2gt - The Raman scattered beam propagates
co-linearly with the reflected laser beam - These mix on the photodiode to produce a
microwave signal this is optical heterodyne
detection. - High (near single photon) sensitivity for
coherent optical signals - Blind to luminescence background
- Allows both amplitude and phase measurements of
the optical signal.
7Simulation of Mn2 in CdTe
Zeeman
Hyperfine, I5/2
Crystal field
Experimental CRESR results from bulk CdTe shown
in red
Biaxial strain or quantum confinement adds
(large) term of this form
8First CRESR result on Mn2 in QWs
- See absorption-like and dispersion-like
components (by analogy with ESR) - At low microwave power, can minimise saturation
effects (no further absorption possible) - Must also avoid microwave heating effects (which
reduce the Mn2 magnetization and shift the
excitonic band gap so that the optical resonance
condition is lost) - Heating is most efficient at the spin resonance
condition (where microwave absorption is strong).
absorption
dispersion
9CRESR from 3 SQWs in one structure
- No sign of any hyperfine structure or crystal
field effects in contrast to dilute bulk
CdMnTe, we only see a single Lorentzian line - Crystal field is now dominated by axial term
representing quantum confinement and strain
effects (with inhomogeneous broadening) - Hyperfine effects are not resolved because of the
relatively high Mn concentration (x 1) which
leads to interactions between Mn ions - Hence, absence of fine structure is not
surprising.
10Selectivity and sensitivity of CRESR
- Signals just discussed came from 3 different QWs
of the same heterostructure - We are able to select these because of their
different resonance energies can demonstrate
this by tuning the laser through the excitonic
transitions of the set of QWs (the magnetic field
is kept at the spin resonance field, 1.2 T) - Also establishes sensitivity is high single QW
with 1 Mn gives SNR of 201
45Å
78Å
301Å
11Summary
- Reviewed SFRS of Mn2.
- Introduced coherent Raman-detected ESR.
- Reviewed Mn2 in bulk CdTe.
- Presented first results of application of CRESR
to a magnetic semiconductor quantum well fine
structure not observed but sensitivity and
selectivity demonstrated. - thanks to EPSRC, Royal Society, INTAS, NATO