![]() ![]() In addition to their practical benefits, luxury duvet covers can also transform the look of your bedroom. Transform Your Bedroom with Luxe Duvet Covers From thick quilted coverlets to plush bedding pillows and warm, sumptuous throws, we master the art of indulgent comfort. They come in a range of colors, patterns, and textures, so you can find the perfect match for your personal style and bedroom decor. Z Gallerie’s exclusive selection of chic bedding is made with high-quality materials that not only feel soft and luxurious but also provide superior durability and longevity. A higher thread count generally indicates a higher-quality product, but keep in mind that thread count isn't the only factor to consider when choosing a duvet cover. Egyptian cotton is known for its luxurious feel and durability, while microfiber is a more affordable option that still offers a soft and comfortable texture. When choosing a duvet cover, consider the material and thread count. One of the easiest ways to transform your bed and elevate your bedroom decor is by investing in luxe bedding.Ĭhoose the Best Material and Thread Count for Your Duvet Upgrade Your Bedding with Luxury Duvet CoversĪ bed is often the centerpiece of any bedroom, and the right bedding can make all the difference in creating a space that feels both comfortable and stylish. get_counts( print ( ' \n H Z H when qubit is 1 \n ' ) print ( 'RESULT: ' ,counts, ' \n ' ) # print ( 'Press any key to close' ) input() job_monitor(job) counts = job. measure(q,c) job = execute(circuit, backend, shots = 100 ) print ( ' \n Executing. x(q) # Used to initialise qubit to 1 circuit. get_counts( print ( ' \n H Z H when qubit is 0 \n ' ) print ( 'RESULT: ' ,counts, ' \n ' ) # H Z H when qubit is 1 # circuit = QuantumCircuit(q,c) circuit. get_counts( print ( ' \n H H \n ' ) print ( 'RESULT: ' ,counts, ' \n ' ) # H Z H when qubit is 0 # circuit = QuantumCircuit(q,c) circuit. get_counts( print ( ' \n Z when qubit is 1 \n ' ) print ( 'RESULT: ' ,counts, ' \n ' ) # H H # circuit = QuantumCircuit(q,c) circuit. ![]() get_counts() print ( ' \n Z when qubit is 0 \n ' ) print ( 'RESULT: ' ,counts, ' \n ' ) # Z gate when qubit is 1 # circuit = QuantumCircuit(q,c) circuit. measure(q,c) # Measuring qubit job = execute(circuit, backend, shots = 100 ) print ( ' \n Executing. get_backend( 'ibmq_qasm_simulator' ) q = QuantumRegister( 1, 'q' ) c = ClassicalRegister( 1, 'c' ) # Z gate when qubit is 0 # circuit = QuantumCircuit(q,c) circuit. get_provider(hub = 'ibm-q' ) backend = provider. enable_account( 'Enter API token here' ) provider = IBMQ. Print ( ' \n Z gate tutorial' ) print ( '-' ) from qiskit import QuantumRegister from qiskit import ClassicalRegister from qiskit import QuantumCircuit, execute,IBMQ from import job_monitor IBMQ. Once you have it copy and paste in to the IBMQ.enable_account('Enter API token here') function in the code. Note: For this tutorial you will need an API token which you can get by registering here: This is extremely useful as it means even though our qubit is in superposition we can conserve information within the qubit.Īs such it is used in many important quantum algorithms such as in Superdense coding where we encode 2 classical bits in 1 qubit. However if we apply a Z-gate between those two Hadamard gates it flips the phase 180 degrees and as such when measured it will not be back in its initialised state but the opposite. If we apply the Hadamard gate again then it flips it back to |0〉when measured. Hence HH = I where I just means identity.Įxample: if we have our qubit set to |0〉and apply a Hadamard gate it will go in to a superposition of states. However if we apply a Hadamard gate again and then measure then it returns back from a superposition to its initialised state. When we apply a Hadamard gate to a qubit it puts it in to a superposition of states such that when measured it could be |0〉 or |1〉 with equal probability. If we initialise our qubit to |1〉 and use the phase flip circuit we will get a |0〉 instead. ![]() If we initialise our qubit to |0〉 and use the phase flip circuit above then we will get |1〉 when measured
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