Single defect centres in diamond: A review
... at 1344 cm–1. The centre is at a C3v symmetry site. It is a deep electron donor, probably 1.7 eV below the conduction band edge. There is an EPR signal associated with this defect, called P1, which identifies it to be an electron paramagnetic system with S = 1/2 ground state [17]. Nitrogen aggregate ...
... at 1344 cm–1. The centre is at a C3v symmetry site. It is a deep electron donor, probably 1.7 eV below the conduction band edge. There is an EPR signal associated with this defect, called P1, which identifies it to be an electron paramagnetic system with S = 1/2 ground state [17]. Nitrogen aggregate ...
ELECTROSTATIC LATTICE for srEDM
... realized in COSY ring Disadvantage: the high requirement to stability of frf 24. Mai 2017 ...
... realized in COSY ring Disadvantage: the high requirement to stability of frf 24. Mai 2017 ...
Section 6 Raman Scattering (lecture 10)
... be scattered (approx. 1 in 107 in a transparent medium). This is not due to defects or dust but a molecular effect which provides another way to study energy levels. This scattering may be: ...
... be scattered (approx. 1 in 107 in a transparent medium). This is not due to defects or dust but a molecular effect which provides another way to study energy levels. This scattering may be: ...
Ultrashort-Pulse Generation and Ultrafast Phenomena
... 13]. However, MBE has disadvantages including high complexity and cost as well as lattice matching constraints that limit material choice. Recently we have developed non-epitaxially grown saturable absorber devices and applied them to self-starting KLM in a Ti:Al2O3 laser [14]. The devices consist o ...
... 13]. However, MBE has disadvantages including high complexity and cost as well as lattice matching constraints that limit material choice. Recently we have developed non-epitaxially grown saturable absorber devices and applied them to self-starting KLM in a Ti:Al2O3 laser [14]. The devices consist o ...
1 Introduction to quantum mechanics
... quantum mechanics of nuclear spins is quite straightforward and many useful calculations can be done by hand, quite literally "on the back of an envelope". This simplicity comes about from the fact that although there are a very large number of molecules in an NMR sample they are interacting very we ...
... quantum mechanics of nuclear spins is quite straightforward and many useful calculations can be done by hand, quite literally "on the back of an envelope". This simplicity comes about from the fact that although there are a very large number of molecules in an NMR sample they are interacting very we ...
optical pumping of rubidium
... corresponding Zeeman levels is forced and, as a result, a deviation from pumping equilibrium. In the other case, the frequency of the irradiating HF field can be slowly varied at constant magnetic field strength. Here, the absorption changes each time ∆E = hf reaches the spacing between neighbouring ...
... corresponding Zeeman levels is forced and, as a result, a deviation from pumping equilibrium. In the other case, the frequency of the irradiating HF field can be slowly varied at constant magnetic field strength. Here, the absorption changes each time ∆E = hf reaches the spacing between neighbouring ...
letter
... mechanics of nuclear spins is quite straightforward and many useful calculations can be done by hand, quite literally "on the back of an envelope". This simplicity comes about from the fact that although there are a very large number of molecules in an NMR sample they are interacting very weakly wit ...
... mechanics of nuclear spins is quite straightforward and many useful calculations can be done by hand, quite literally "on the back of an envelope". This simplicity comes about from the fact that although there are a very large number of molecules in an NMR sample they are interacting very weakly wit ...