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(Solved): Consider the following 2D hexagonal Bravais lattice with lattice constant avec(a_(1)) and vec(a_(2)) ...



Consider the following 2D hexagonal Bravais lattice with lattice constant avec(a_(1)) and vec(a_(2)) vec(b_(1)) and vec(b_(2)). bvec(b_(1)),vec(b_(2)), and the FBZ in the reciprocal lattice. You will see that the reciprocal lattice is also hexagonal. What is the lattice constant |vec(b_(1))| or |vec(b_(2))| of the reciprocal lattice? cE(k_(x),k_(y))=+-ℏv_(F)\sqrt(k_(x)^(2)+k_(y)^(2)), where v_(F) is a characteristic velocity equal to 10^(8)c(m)/(s) for graphene. Sketch E(k_(x),k_(y)) in the 2D k-space. dg(E)=(g_(s)g_(v))/(2\pi ((h)v_(F))^(2))|E|, where g_(s)=2 is the spin degeneracy of each (k_(x),k_(y)) state and g_(v) (valley degeneracy) =2 is the number of inequivalent copies of the E-k dispersion relationship in k-space. eE =0, the conduction electron density in graphene is n_(2D)= (\pi )/(6)((k_(B)T)/(ℏv_(F)))^(2). This is the intrinsic sheet electron density of graphene, which is the lowest achievable density of conduction electrons at temperature T. You may use the result \int_0^(\infty ) (E)/(1+exp((E)/(\alpha )))dE=(\pi ^(2)\alpha ^(2))/(12).


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