```
from qiskit import *
from qiskit.tools.visualization import plot_histogram
import numpy as np
```

## 1

Show that the Hadamard gate can be written in the following two forms

$$H = \frac{X+Z}{\sqrt{2}} \equiv \exp\left(i \frac{\pi}{2} \, \frac{X+Z}{\sqrt{2}}\right).$$Here $\equiv$ is used to denote that the equality is valid up to a global phase, and hence that the resulting gates are physically equivalent.

Hint: it might even be easiest to prove that $e^{i\frac{\pi}{2} M} \equiv M$ for any matrix whose eigenvalues are all $\pm 1$, and that such matrices uniquely satisfy $M^2=I$.

## 2

The Hadamard can be constructed from `rx`

and `rz`

operations as

For some suitably chosen $\theta$. When implemented for finite $n$, the resulting gate will be an approximation to the Hadamard whose error decreases with $n$.

The following shows an example of this implemented with Qiskit with an incorrectly chosen value of $\theta$ (and with the global phase ignored).

Determine the correct value of $\theta$.

Show that the error (when using the correct value of $\theta$) decreases quadratically with $n$.

```
q = QuantumRegister(1)
c = ClassicalRegister(1)
error = {}
for n in range(1,11):
# Create a blank circuit
qc = QuantumCircuit(q,c)
# Implement an approximate Hadamard
theta = np.pi # here we incorrectly choose theta=pi
for j in range(n):
qc.rx(theta/n,q[0])
qc.rz(theta/n,q[0])
# We need to measure how good the above approximation is. Here's a simple way to do this.
# Step 1: Use a real hadamard to cancel the above approximation.
# For a good approximatuon, the qubit will return to state 0. For a bad one, it will end up as some superposition.
qc.h(q[0])
# Step 2: Run the circuit, and see how many times we get the outcome 1.
# Since it should return 0 with certainty, the fraction of 1s is a measure of the error.
qc.measure(q,c)
shots = 20000
job = execute(qc, Aer.get_backend('qasm_simulator'),shots=shots)
try:
error[n] = (job.result().get_counts()['1']/shots)
except:
pass
plot_histogram(error)
```