o Problem 1 [level of difficulty: easy but tedious): Consider the 3-qubit state (4) = 11010) + V3|100), and suppose that we perform an observation in the following manner: The leftmost qubit is observed in the standard computational basis 10), (1). . The middle qubit is observed in the Hadamard basis (+) = ta 10) + tal1), 1-) = tal0) T211). The rightmost qubit is observed in the basis |+I) = Da 10) + 13/1),|-1) = tz10) ja 1). For each combination ijk, where i E {0,1}, je {+, - }, k {+1,-1}, determine the probability of observing lijk). Note that the calculations could be tedious but conceptually easy. Hint: For the middle qubit, express (0) and 1) in terms of |+) and (-) respectively, and similarly for the rightmost qubit, express (0) and (1) in terms of |+I) and (-1) respectively. Then, expand the tensor products. o Problem 1 [level of difficulty: easy but tedious): Consider the 3-qubit state (4) = 11010) + V3|100), and suppose that we perform an observation in the following manner: The leftmost qubit is observed in the standard computational basis 10), (1). . The middle qubit is observed in the Hadamard basis (+) = ta 10) + tal1), 1-) = tal0) T211). The rightmost qubit is observed in the basis |+I) = Da 10) + 13/1),|-1) = tz10) ja 1). For each combination ijk, where i E {0,1}, je {+, - }, k {+1,-1}, determine the probability of observing lijk). Note that the calculations could be tedious but conceptually easy. Hint: For the middle qubit, express (0) and 1) in terms of |+) and (-) respectively, and similarly for the rightmost qubit, express (0) and (1) in terms of |+I) and (-1) respectively. Then, expand the tensor products