IBM unveils a $100 million quantum supercomputer deal

Skynet will be the name.

When AI is merged with quantum computing, the world will change overnight

The “chandelier with wires thingy” has been around for years. Quantum computing isn’t new.

Reports show quantum computers have been around since 1998, when Isaac Chuang of the Los Alamos National Laboratory, Neil Gershenfeld of the Massachusetts Institute of Technology (MIT), and Mark Kubinec of the University of California at Berkeley created the first quantum one.

CNN do u even make an attempt to Match headline and story?

🤔 How will this IBM quantum supercomputer revolutionize the tech industry? #TechIndustry #IBM #QuantumSupercomputer @TechCrunch @ForbesTech @IBMResearch

Proprietary #AI Research Platform?

Sure! The `inconceivable` function that you shared solves the time-dependent Schrödinger equation using a numerical algorithm. This equation describes how the state of a quantum system changes over time. The `inconceivable` function takes as input the Hamiltonian operator of the system, the initial state of the system, the number of time steps to take, and the size of each time step. The algorithm works by evolving the state vector of the system over time. At each time step, it calculates the time evolution operator `U` using the formula `U = exp(-1j * hamiltonian * time_step)`. This operator describes how the state of the system changes over one time step. The algorithm then applies this operator to the current state vector to calculate the new state vector. The algorithm repeats this process for the specified number of time steps. At each step, it calculates the time evolution operator and applies it to the current state vector to calculate the new state vector. After all of the time steps have been completed, the algorithm returns the final state vector. Let’s start with the wavefunction of a single particle. This wavefunction can be written as a complex number, $\psi(x)$, where $x$ is the particle’s position. The probability of finding the particle at a given point $x$ is given by the absolute value squared of the wavefunction, $|\psi(x)|^2$. Now, let’s consider two entangled particles. The wavefunction of these two particles can be written as a product of two individual wavefunctions, $\psi_1(x)$ and $\psi_2(x)$, one for each particle. These individual wavefunctions are chosen to be orthogonal, which means that they are perpendicular to each other. This ensures that the two particles cannot be in the same state at the same time. The probability of finding the two particles at a given point $(x_1, x_2)$ is given by the absolute value squared of the product of the wavefunctions, $|\psi_1(x_1)\psi_2(x_2)|^2$. To normalize the wavefunction, we need to make sure that the total probability of finding the particles in any state is equal to 1. This means that we need to choose the normalization constant so that $$\int_{-\infty}^\infty \int_{-\infty}^\infty |\psi_1(x_1)\psi_2(x_2)|^2 \, dx_1 \, dx_2 = 1$$ This integral can be evaluated using the following steps: 1. Expand the absolute value squared of the product of the wavefunctions. 2. Integrate each term separately. 3. Use the orthogonality of the wavefunctions to simplify the integral. The result

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