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y state with a field dependent y component of the nesting vector which was suggested to exist in a narrow field range for certain values of electron coupling constants (Ref. 11). This, however, does not affect the physical nature of the described phenomenon
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y state with a field dependent y component of the nesting vector which was suggested to exist in a narrow field range for certain values of electron coupling constants (Ref. 11). This, however, does not affect the physical nature of the described phenomenon.
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Based on geometrical considerations, one can roughly estimate the upper limit for the field, at which closed pockets are formed, from the condition: (Formula presented)
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Based on geometrical considerations, one can roughly estimate the upper limit for the field, at which closed pockets are formed, from the condition: (Formula presented).
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The coupling of the nesting vector to very strong dHvA oscillations of the Q2D carriers was proposed to be a reason of a hysteresis in the high-field magnetization at θ 0°
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