Rotational quantum number and vibronic symmetry of nitrogen dioxide excited with visible light in the region of 563-566 nm: optical-optical double resonance measurement and spin-orbit interaction between 2B2 and 2A2 vibronic states

1993 ◽  
Vol 97 (35) ◽  
pp. 8889-8894 ◽  
Author(s):  
Kaoru Aoki ◽  
Hidekazu Nagai ◽  
Kennosuke Hoshina ◽  
Kazuhiko Shibuya
1986 ◽  
Vol 85 (8) ◽  
pp. 4297-4303 ◽  
Author(s):  
Stephen L. Coy ◽  
Kevin K. Lehmann ◽  
Frank C. De Lucia

1994 ◽  
Vol 14 (1-3) ◽  
pp. 119-129
Author(s):  
Kazuhiko Shibuya ◽  
Tadasi Kusumoto ◽  
Hidekazu Nagai

Optical–optical double resonance (OODR) spectroscopy has been applied to the rotational and vibronic analysis of the thirty nine eigenstates of NO2 existing in the energy region of 16,980–17,124 cm-1 above the ground state. These excited states are concluded to be the mixed states of NO2 generated by spin-orbit and/or orbital-rotation interaction between the B2 and A1 vibronic levels. The mixing mechanism of the excited states is discussed in terms of available information on the visible excited states of NO2.


Author(s):  
J. Nitta

This chapter focuses on the electron spin degree of freedom in semiconductor spintronics. In particular, the electrostatic control of the spin degree of freedom is an advantageous technology over metal-based spintronics. Spin–orbit interaction (SOI), which gives rise to an effective magnetic field. The essence of SOI is that the moving electrons in an electric field feel an effective magnetic field even without any external magnetic field. Rashba spin–orbit interaction is important since the strength is controlled by the gate voltage on top of the semiconductor’s two-dimensional electron gas. By utilizing the effective magnetic field induced by the SOI, spin generation and manipulation are possible by electrostatic ways. The origin of spin-orbit interactions in semiconductors and the electrical generation and manipulation of spins by electrical means are discussed. Long spin coherence is achieved by special spin helix state where both strengths of Rashba and Dresselhaus SOI are equal.


2019 ◽  
Vol 3 (6) ◽  
Author(s):  
J. N. Nelson ◽  
J. P. Ruf ◽  
Y. Lee ◽  
C. Zeledon ◽  
J. K. Kawasaki ◽  
...  

2021 ◽  
Vol 103 (19) ◽  
Author(s):  
Miguel J. Carballido ◽  
Christoph Kloeffel ◽  
Dominik M. Zumbühl ◽  
Daniel Loss

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