Quantum energy teleportation

There are two main factors involved in how QET works: how energy is transferred from Alice to Bob, and how Bob can extract energy from his spin.

File:Spin chain3.png

QET is studied through analyzing spin chain models. A spin chain is a type of model where a one dimensional chain of sites are assigned certain spin value at each site, typically +1/2 or -1/2 when considering spin-1/2. The spin of one individual site can interact with the spin of its adjacent neighbours, causing the entire system to be coupled together.{{cite report |type=Preprint |last=Crichigno |first=Marcos |date=23 July 2024 |title=Quantum Spin Chains and Symmetric Functions |arxiv=2404.04322 }}

Spin chains are useful for QET due to the fact that they can be entangled even in the ground state. This means that even without external energy being added to the system, the ground state exhibits quantum correlations across the chain. Alice and Bob are both in possession of an entangled state from a spin chain system. This can provide a rudimentary explanation of how energy can be transferred from Alice's spin to Bob's spin, since any action on Alice's spin can have an effect on Bob's spin.{{cite report |type=Preprint |last=Hotta |first=Mashahiro |date=20 January 2011 |title=Quantum Energy Teleportation: An Introductory Review |arxiv=1101.3954 }}

The other key component to understanding the QET mechanism is vacuum fluctuations and the presence of negative energy density regions within the energy distribution of a quantum mechanical system. Vacuum fluctuations are a consequence of the Heisenberg uncertainty principle where the energy-time uncertainty principle,

File:Vacuum fluctuations3.png

$\backslash Delta\; E\; \backslash Delta\; t\; \backslash geq\; \backslash frac\{1\}\{2\}\backslash hbar$ , states that there is uncertainty in energy over a time span $\backslash Delta\; t$. So, the energy will fluctuate about the zero-point energy of the state.

The vacuum fluctuations in certain regions can have lower amplitude fluctuations due to the effect of local operations. These regions possess a negative energy density since the vacuum fluctuations already represent the zero-energy state. Therefore, fluctuations of lower amplitude relative to the vacuum fluctuations represent a negative energy density region. Since the entire vacuum state still has zero-energy, there exist other regions with higher vacuum fluctuations with a positive energy density.

Negative energy density in the vacuum fluctuations plays an important role in QET since it allows for the extraction of energy from the vacuum state. Positive energy can be extracted from regions of positive energy density which can be created by regions of negative density region elsewhere in the vacuum state.

The QET process is considered over short time scales, such that the Hamiltonian of the spin chain system is approximately invariant with time. It is also assumed that local operations and classical communications (LOCC) for the spins can be repeated several times within a short time span. Alice and Bob share entangled spin states in the ground state $|g\backslash rangle$ with correlation length $\backslash ell$. Alice is located at site $n\_A$ of the spin chain system and Bob is located at site $n\_B$ of the spin chain system such that Alice and Bob are far away from each other, $|n\_A\; -\; n\_B|\; \backslash gg\; 1$.{{cite report |type=Preprint |last=Hotta |first=Masahrio |date=22 Dec 2008 |title=Quantum Energy Teleportation in Spin Chain Systems |arxiv=0803.0348 }}

File:QET4.png

Conceptually, the QET protocol can be described by three steps:

1. Alice performs a local measurement on her spin at site $n\_A$, measuring eigenvalue $\backslash mu$. When Alice acts on her spin with the local operator, energy $E\_A$ is inputted into the state.
2. Alice then communicates to Bob over a classical channel what her measurement result $\backslash mu$ was. It is assumed that over the time the classical message is travelling that Alice and Bob's state does not evolve with time.
3. Based on the measurement Alice got on her spin $\backslash mu$, Bob applies a specific local operator to his spin located at site $n\_B$. After the application of the local operator, the expectation value of the Hamiltonian at this site $\backslash hat\{H\}\_\{n\_B\}$ is negative. Since the expectation of $\backslash hat\{H\}\_\{n\_B\}$ is zero before Bob's operation, the negative expectation value of $\backslash hat\{H\}\_\{n\_B\}$ after the local operation implies energy was extracted at site $n\_B$ while the operation was being applied.

Intuitively, one would not expect to be able to extract energy from the ground state in such a manner. However, this protocol allows energy to be teleported from Alice to Bob, despite Alice and Bob sharing entangled spin states in the ground state.

The QET protocol can be worked out mathematically. The derivation in this section follows the work done by Masahiro Hotta in "Quantum Energy Teleportation in Spin Chain Systems". Consider Alice's spin at site $n\_A$ in a spin chain where each spin is entangled in ground state $|g\backslash rangle$. For a Hermitian unitary local operator $\backslash hat\{\backslash sigma\}\_A\; =\; \backslash vec\{u\}\_A\; \backslash cdot\; \backslash vec\{\backslash sigma\}\_\{n\_A\}$, where $\backslash vec\{u\}\_A$ represents a 3D unit vector and $\backslash vec\{\backslash sigma\}\_\{n\_A\}$ is the Pauli spin matrix vector at site $n\_A$, the eigenvalues are $(-1)^\backslash mu$ with $\backslash mu\; =\; 0,1$. Alice can perform a measurement on spin at site $n\_A$ using this local operator to measures $\backslash mu\; =\; 0\; \backslash text\{\; or\; \}\; 1$. The expression for $\backslash hat\{\backslash sigma\}\_A$ has spectral expansion $\backslash hat\{\backslash sigma\}\_A\; =\; \backslash sum\_\{\backslash mu\; =\; 0,\; 1\}\; (-1)^\backslash mu\; \backslash hat\{P\}\_A(\backslash mu)$ where $\backslash hat\{P\}\_A(\backslash mu)$ is a projective operator which projects onto the eigensubspace with $\backslash mu$. After Alice has made the measurement with the $\backslash hat\{\backslash sigma\}\_A$ operator, the spin is left in the post-measurement state $\backslash frac\{1\}\{\backslash sqrt\{p\_A(\backslash mu)\}\}\; \backslash hat\{P\}\_A(\backslash mu)\; |g\backslash rangle$ where $p\_A(\backslash mu)\; =\; \backslash langle\; g|\; \backslash hat\{P\}\_A(\backslash mu)\; |g\backslash rangle$. This is a mixed quantum state with density matrix: $$\backslash begin\{align\}$$

\hat{\rho}' &= \sum_{\mu=0,1}p_A(\mu)\frac{1}{\sqrt{p_A(\mu)}}\hat{P}_A(\mu)|g \rangle \langle g| \hat{P}_A(\mu) \frac{1}{\sqrt{p_A(\mu)}} \\

&= \hat{P}_A(\mu) |g \rangle \langle g| \hat{P}_A(\mu).

\end{align}This density matrix satisfies the relation:

$\backslash text\{Tr\}\_\{n\_A\}[\backslash rho\text{'}]\; =\; \backslash text\{Tr\}\_\{n\_A\}[|g\backslash rangle\; \backslash langle\; g|]$

which shows that the quantum fluctuation of $\backslash rho\text{'}$ is the same as that of the ground state except at site $n\_A$. This measurement requires Alice to input energy $E\_A$ into the spin chain. Since the ground state has zero energy, $E\_A$ is related by the difference in energy between the final quantum state $\backslash rho\text{'}$ and the initial ground state $|g\backslash rangle$:$$E\_A\; =\; \backslash text\{Tr\}\; [\backslash hat\{\backslash rho\}\text{'}\; \backslash hat\{H\}]\; -\; \backslash langle\; g\; |\; \backslash hat\{H\}\; |\; g\; \backslash rangle\; =\; \backslash sum\_\{\backslash mu=0,1\}\; \backslash langle\; g\; |\; \backslash hat\{P\}\_A(\backslash mu)\; \backslash hat\{H\}\; \backslash hat\{P\}\_A(\backslash mu)\; |\; g\; \backslash rangle.$$The energy Alice needs to input is non-negative since $\backslash hat\{H\}$ is non-negative. $\backslash hat\{H\}$ is shown to be non-negative in the source material. This is an important result of the measurement process as the point of the QET protocol is for Alice to inject a positive quantity of energy into the spin chain.

The Hamiltonian for the spin chain system $\backslash hat\{H\}$ can be expressed as the sum of the local energy operators $\backslash hat\{T\_n\}$ over all $n$ spins: $\backslash hat\{H\}\; =\; \backslash sum\_n\; \backslash hat\{T\}\_n$. The local energy operators $\backslash hat\{T\_n\}$ can be shifted by adding constants such that the expectation value of the local energy operators are each zero, $\backslash langle\; g\; |\; \backslash hat\{T\}\_n\; |\; g\; \backslash rangle\; =\; 0$. Due to entanglement, the ground state $|g\; \backslash rangle$ is not an eigenstate of $\backslash hat\{T\_n\}$. Since the expectation value of the local energy operators are zero, it implies that the lowest eigenvalue of $\backslash hat\{T\_n\}$ must be negative. The expectation value of $\backslash hat\{T\_n\}$ involves eigenstates of $\backslash hat\{T\_n\}$ with positive and negative energy densities, but will average to 0 across all eigenstates. Therefore, some of the spins in the spin chain that possess a negative energy density lead to spins possessing positive energy density to balance them out. This implies that energy can be withdrawn from certain spin sites with positive energy density, which is the process Bob will use to receive the teleported energy from Alice.

Alice then informs Bob of the value of the measurement $\backslash mu$ over a classical channel. The time interval over which this information is transferred is considered to be very short such that the system does not evolve over this time and no emergence of energy flux occurs.

Bob then applies the local unitary $\backslash hat\{U\}\_B(\backslash mu)$ to the spin at site $n\_B$ where $\backslash hat\{U\}\_B(\backslash mu)\; =\; \backslash hat\{I\}\; \backslash text\{cos\}\; \backslash theta\; +\; i\; (-1)^\backslash mu\; \backslash hat\{\backslash sigma\}\_B\; \backslash text\{sin\}\; \backslash theta$. Here $\backslash hat\{\backslash sigma\}\_B\; =\; \backslash vec\{u\}\_B\; \backslash cdot\; \backslash vec\{\backslash sigma\}\_\{n\_B\}$ where $\backslash vec\{u\}\_B$ is a 3D unit vector and $\backslash vec\{\backslash sigma\}\_\{n\_B\}$ is the Pauli spin matrix vector at site $n\_B$. Two real coefficients are introduced $\backslash xi\; =\; \backslash langle\; g\; |\; \backslash hat\{\backslash sigma\}\_B\; \backslash hat\{H\}\; \backslash hat\{\backslash sigma\}\_B\; |\; g\; \backslash rangle$ and $\backslash eta\; =\; \backslash langle\; g\; |\; \backslash hat\{\backslash sigma\}\_A\; \backslash dot\{\backslash hat\{\backslash sigma\}\}\_B\; |\; g\; \backslash rangle$, where $\backslash dot\{\backslash hat\{\backslash sigma\}\}\_B\; =\; i\; [\backslash hat\{H\}\_\{n\_B\},\; \backslash hat\{\backslash sigma\}\_B]$, which can be used to define the real angle parameter $\backslash theta$ by $\backslash text\{cos\}\; (2\; \backslash theta)\; =\; \backslash frac\{\backslash xi\}\{\backslash sqrt\{\backslash xi^2\; +\; \backslash eta^2\}\}$ and $\backslash text\{sin\}\; (2\; \backslash theta)\; =\; -\backslash frac\{\backslash eta\}\{\backslash sqrt\{\backslash xi^2\; +\; \backslash eta^2\}\}$. Using $[\backslash hat\{T\}\_n,\; \backslash hat\{\backslash sigma\}\_B]\; =\; 0$ for $|n\; -\; n\_B|\; >\; L$, $\backslash dot\{\backslash hat\{\backslash sigma\}\}\_B$ can be expressed as $\backslash dot\{\backslash hat\{\backslash sigma\}\}\_B\; =\; i[\backslash hat\{H\},\; \backslash hat\{\backslash sigma\}\_B]$. $\backslash hat\{T\_n\}$ refers to the local energy at site $n$.

The full derivation can be found in the source material. Essentially, Bob's application of the local unitary $\backslash hat\{U\}\_B(\backslash mu)$ leaves his state in the quantum state $\backslash hat\{\backslash rho\}$. By using the relations for $\backslash theta$ and other simplifications, the expectation value of the energy at site $n\_B$ can be expressed as $\backslash text\{Tr\}\; [\backslash hat\{\backslash rho\}\; \backslash hat\{H\}\_\{n\_B\}]$ or$$\backslash text\{Tr\}[\backslash hat\{\backslash rho\}\; \backslash hat\{H\}\_\{n\_B\}]\; =\; \backslash frac\{1\}\{2\}\; \backslash left[\; \backslash xi\; -\; \backslash sqrt\{\backslash xi^2\; +\; \backslash eta^2\}\; \backslash right].$$If $\backslash eta\; \backslash neq\; 0$ then $\backslash text\{Tr\}\; [\backslash hat\{\backslash rho\}\; \backslash hat\{H\}\_\{n\_B\}]$ becomes negative. Before Bob acts with the local unitary $\backslash hat\{U\}\_B(\backslash mu)$, the energy around Bob is zero: $\backslash text\{Tr\}[\backslash hat\{\backslash rho\}\text{'}\; \backslash hat\{H\}\_\{n\_B\}]\; =\; 0$. This implies that some positive energy $E\_B$ must be emitted from the spin chain as from the local energy conservation around site $n\_B$: $E\_B\; +\; \backslash text\{Tr\}[\backslash hat\{\backslash rho\}\; \backslash hat\{H\}\_\{n\_B\}]\; =\; \backslash text\{Tr\}[\backslash hat\{\backslash rho\}\text{'}\; \backslash hat\{H\}\_\{n\_B\}]\; =\; 0$. Which then follows that:$$\backslash begin\{align\}$$

E_B &= \text{Tr}[\hat{\rho}' \hat{H}_{n_B}] - \text{Tr}[\hat{\rho} \hat{H}_{n_B}] \\

&= \frac{1}{2} \left[ \sqrt{\xi^2 + \eta^2} - \xi \right].

\end{align}So some positive quantity of energy $E\_B$ has been extracted from site $n\_B$, completing the QET protocol.

One of the constraints on the protocol is that Alice and Bob must share an entangled state. This can be proved mathematically. If the ground state is separable and can be expressed as $|g\; \backslash rangle\; =\; |g\; \backslash rangle\_A\; \backslash otimes\; |g\; \backslash rangle\_B$ and the relations $\backslash dot\{\backslash hat\{\backslash sigma\}\}\_B\; =\; i[H,\; \backslash hat\{\backslash sigma\}\_B]$ and $\backslash hat\{H\}\; |g\; \backslash rangle\; =\; 0$ are used then it follows that:$$\backslash begin\{align\}$$

\eta &= \langle g | \hat{\sigma}_A \dot{\hat{\sigma}}_B |g \rangle = \langle g | \hat{\sigma}_A |g \rangle \langle g |\dot{\hat{\sigma}}_B |g \rangle \\

&=i\langle g | \hat{\sigma}_A |g \rangle \langle g | (\hat{H} \hat{\sigma}_B - \hat{\sigma}_B \hat{H}) |g \rangle = 0.

\end{align}Therefore, Alice and Bob must share an entangled state for energy to be transported from Alice to Bob otherwise $\backslash eta$ vanishes which causes $E\_B$ to vanish.

One could postulate that Alice could withdraw the energy she puts into the system when measuring $\backslash hat\{\backslash sigma\}\_A$, $E\_A$, thus making the energy Bob extracts, $E\_B$, have zero-cost. Mathematically, this is not possible. First, when Alice measures $\backslash hat\{\backslash sigma\}\_A$ at site $n\_A$ the entanglement between the spin at site $n\_A$ and the rest of the chain is broken since Alice has collapsed the local state. So, for Alice to extract the energy she first deposited to the system during the measurement process she must first restore the ground state. This implies that Alice would have to recreate the entanglement between the spin at site $n\_A$ and the rest of the chain which is not possible with only local operators. To recreate the entanglement, Alice would need to use non-local operators which inherently require energy.{{cite journal |last1=Andreadakis |first1=Faidon |last2=Dallas |first2=Emanuel |last3=Zanardi |first3=Paolo |title=Operator space entangling power of quantum dynamics and local operator entanglement growth in dual-unitary circuits |journal=Physical Review A |date=12 November 2024 |volume=110 |issue=5 |page=052416 |doi=10.1103/PhysRevA.110.052416 |arxiv=2406.10206 |bibcode=2024PhRvA.110e2416A }} Therefore, it is impossible for Alice to extract the energy $E\_A$ while only using local operators.

Quantum energy distribution (QED) is a protocol proposed by Masahiro Hotta in "A Protocol for Quantum Energy Distribution" which proposes an extension of QET with quantum key distribution (QKD). This protocol allows an energy supplier $S$ to distribute energy to $M$ consumers denoted by $C\_m$.

The supplier $S$ and any consumer $C\_m$ share common short keys $k$ which are used for identification. Using the short keys $k$, $S$ and $C\_m$ can perform secure QKD which allows $S$ to send classical information to the consumers. It is assumed that $S$ and $C\_m$ share a set of many spin states in the ground state $|g\; \backslash rangle$. The protocol follows six steps:

1. $S$ performs a local measurement of the observable $\backslash hat\{U\}\_S\; =\; \backslash sum\_\{\backslash mu=0,1\}\; (-1)^\backslash mu\; \backslash hat\{P\}\_S(\backslash mu)$ on the ground state $|g\; \backslash rangle$ and measures $\backslash mu$. $S$ must input energy $E\_S\; =\; \backslash sum\_\{\backslash mu=0,1\}\; \backslash langle\; g\; |\; \backslash hat\{P\}\_S(\backslash mu)\; \backslash hat\{H\}\; \backslash hat\{P\}\_S(\backslash mu)\; |\; g\; \backslash rangle$ into the spin chain.
2. $S$ confirms the identity of $C\_m$ through use of the shared secret short keys $k$.
3. $S$ and $C\_m$ share pseudo-random secret keys $K$ by use of a QKD protocol.
4. $S$ encodes the measurement result $\backslash mu$ using secret key $K$ and sends it to $C\_m$.
5. $C\_m$ decodes the measurement result $\backslash mu$ using secret key $K$.
6. $C\_m$ performs the local unitary operation $\backslash hat\{V\}\_m(\backslash mu)$ to their spin. $C\_m$ receives energy $E\_m\; =\; \backslash frac\{1\}\{2\}\; \backslash left[\; \backslash sqrt\{\backslash xi\_m^2\; +\; \backslash eta\_m^2\}\; -\; \backslash xi\_m\; \backslash right]$ where $\backslash xi\_m\; =\; \backslash langle\; g|\; \backslash hat\{U\}^\backslash dagger\_m\; \backslash hat\{H\}\; \backslash hat\{U\}\_m\; |g\; \backslash rangle$, $\backslash eta\_m\; =\; \backslash langle\; g|\; \backslash hat\{U\}\_s\; \backslash dot\{\backslash hat\{U\}\}\_m\; |g\; \backslash rangle$, $\backslash hat\{U\}\_m\; =\; \backslash vec\{n\}\_m\; \backslash cdot\; \backslash vec\{\backslash sigma\}\_\{n\_\{C\_\{m\}\}\}$, $\backslash dot\{\backslash hat\{U\}\}\_m\; =\; i\; [\backslash hat\{H\}\_\{C\_\{m\}\},\; \backslash hat\{U\}\_m]$, $\backslash vec\{n\}\_m$ is a unit vector, and $\backslash vec\{\backslash sigma\}\_\{n\_\{C\_\{m\}\}\}$ is the Pauli spin matrix vector at site $n\_\{C\_\{m\}\}$.

This process is robust against an unidentified consumer, a thief $D$, at site $n\_D$ attempting to steal energy from the spin chain. After step 6, the post-measurement state is given by $$\backslash hat\{\backslash rho\}\; =\; \backslash sum\_\{\backslash mu=0,1\}\; \backslash left(\; \backslash prod\_m\; \backslash hat\{U\}\_m(\backslash mu)\; \backslash right)\; \backslash hat\{P\}\_S(\backslash mu)\; |g\; \backslash rangle\; \backslash langle\; g|\; \backslash hat\{P\}\_S(\backslash mu)\; \backslash left(\; \backslash prod\_m\; \backslash hat\{U\}^\backslash dagger\_m(\backslash mu)\; \backslash right).$$Since $D$ has no information on $\backslash mu$ and therefore randomly acts with either $\backslash hat\{U\}\_D(0)$ or $\backslash hat\{U\}\_D(1)$ where $\backslash hat\{U\}\_D(\backslash mu)\; =\; \backslash hat\{I\}\; \backslash text\{cos\}\; \backslash theta\; +\; i\; (-1)^\backslash mu\; \backslash vec\{n\}\_D\; \backslash cdot\; \backslash vec\{\backslash sigma\}\_\{n\_\{D\}\}\backslash text\{sin\}\; \backslash theta$. The post-measurement state becomes a sum over the possible guesses D makes of $\backslash mu$, 0 or 1. Taking the expectation value of the localized energy operator $\backslash hat\{H\}\_D$ yields:

$$\backslash text\{Tr\}[\backslash hat\{\backslash rho\}\_D\; \backslash hat\{H\}\_D]\; =\; \backslash frac\{1\}\{2\}\; \backslash sum\_\{\backslash mu=0,1\}\; \backslash langle\; g|\backslash hat\{P\}\_S(\backslash mu)\; \backslash left(\; \backslash prod\_m\; \backslash hat\{U\}^\backslash dagger\_m(\backslash mu)\; \backslash right)\; \backslash hat\{U\}^\backslash dagger\_D(\backslash mu)\; \backslash hat\{H\}\_D\; \backslash hat\{U\}\_D(\backslash mu)\; \backslash left(\; \backslash prod\_m\; \backslash hat\{U\}\_m(\backslash mu)\; \backslash right)\; \backslash hat\{P\}\_S(\backslash mu)\; |g\; \backslash rangle.$$$\backslash hat\{H\}\_D$ is positive semi-definite by definition. This means that all expectation values of $\backslash hat\{H\}\_D$, even the ones altered by $\backslash hat\{U\}\_D(\backslash mu)$, are greater than or equal to zero. At least one of the values in the sum of the trace will be positive, the one where $D$ guesses the wrong value of $\backslash mu$. This is because the operation $\backslash hat\{U\}\_D(\backslash mu)|g\backslash rangle$ will add energy to the system when $\backslash mu$ does not match the value measured by Alice. Therefore, $\backslash text\{Tr\}[\backslash hat\{\backslash rho\}\_D\; \backslash hat\{H\}\_D]\; >\; 0$ which implies that on average $D$ will have to input energy to the spin chains without gain.

This protocol is not perfect as theoretically $D$ could guess $\backslash mu$ on their first attempt, which would be a 50% chance to guess $\backslash mu$ correctly, and would immediately profit energy. However, the idea is that over multiple attempts $D$ will lose energy since the energy output from a correct guess is lower than that of the energy input required when making an incorrect guess.

QET was first experimentally demonstrated in 2023 by Kazuki Ikeda in the publication "Demonstration of Quantum Energy Teleportation on Superconducting Quantum Hardware". The basic QET protocol discussed early was verified using several IBM superconducting quantum computers. Some of the quantum computers that were used include ibmq_lima, and ibm_cairo, and ibmq_jakarta which provided the most accurate results for the experiment. These quantum computers provide two connected qubits with high precision for controlled gate operation. The Hamiltonian used accounted for interactions between the two qubits using the $\backslash hat\{X\}$ and $\backslash hat\{Z\}$ Pauli operators.

The entangled ground state was first prepared using the $\backslash widehat\{\backslash text\{CNOT\}\}$ and $\backslash hat\{R\}\_Y$ quantum gates. Alice then measured her state using the Pauli operator $\backslash hat\{X\}$, injecting energy $E\_0$ into the system. Alice then told Bob her measurement result over a classical channel. The classical communication of measurement results was on the order of 10 nanoseconds and was much faster than the energy propagation timescale of the system. Bob then applied a conditional rotational operation on his qubit dependent on Alice's measurement. Bob then performed a local measurement on his state to extract energy from the system $E\_1$.

The observed experimental values are dimensionless and the energy values correspond to the eigenvalues of the Hamiltonian. For quantum computers, energy scales tend to be limited by the qubit transition frequency which is often on the order of GHz. Therefore, the typical energy scale is on the order of $10^\{-24\}$ Joules. Ikeda experimented with varying the parameters in the Hamiltonian, specifically the local energy $h$ and interaction strength $k$, to see if the QET protocol improved under certain conditions.

For differing experimental parameters, the experimental values for Alice's input energy $E\_0$ was around 1 and matched the experimental results very closely when error mitigation was applied. Bob's extracted energy $E\_1$, for certain experimental parameters, was observed to be negative when error mitigation was applied. This indicates that the QET protocol was successful for certain experimental parameters. Depending on the experimental parameters, Bob would receive around 1-5% of Alice's inputted energy.

Quantum computers are currently the most viable platform for experimentally realizing QET. This is mainly due to their ability to implement quantum error correction. Quantum error correction is important specifically for implementing QET protocols experimentally due to the high precision needed to calculate the negative energy Bob receives in the QET protocol. Error correction in this experiment greatly improved the amount of energy Bob could extract from the system. In some cases without error correction, Bob's extracted energy would be positive, indicating the QET protocol did not work. However after error correction, these values could be brought closer to the experimental values and in some cases even become negative, causing the QET protocol to function. The quantum error correction employed in this experiment allowed Ikeda to observe negative expectation values of the extracted energy $E\_1$, which had not been experimentally observed before. High precision is also required for experimental implementation of QET due to the subtle effects of negative energy density. Since negative energy densities are a consequence of vacuum fluctuations, they can easily be overshadowed by measurement noise in the instrumentation. So, higher precision can lead to better distinguishability between negative energy signals and noise.

• Quantum teleportation
• Quantum entanglement
• Spin chains
• Quantum key distribution
• Quantum information science

{{Reflist}}

• {{cite journal |last1=Hotta |first1=Masahiro |title=Quantum measurement information as a key to energy extraction from local vacuums |journal=Physical Review D |date=8 August 2008 |volume=78 |issue=4 |page=045006 |doi=10.1103/PhysRevD.78.045006 |arxiv=0803.2272 |bibcode=2008PhRvD..78d5006H }}
• {{cite journal |last1=Hotta |first1=Masahiro |title=Quantum Energy Teleportation in Spin Chain Systems |journal=Journal of the Physical Society of Japan |date=15 March 2009 |volume=78 |issue=3 |pages=034001 |doi=10.1143/JPSJ.78.034001 |arxiv=0803.0348 |bibcode=2009JPSJ...78c4001H }}
• {{cite journal |last1=Hotta |first1=Masahiro |last2=Matsumoto |first2=Jiro |last3=Yusa |first3=Go |title=Quantum energy teleportation without a limit of distance |journal=Physical Review A |date=13 January 2014 |volume=89 |issue=1 |page=012311 |doi=10.1103/PhysRevA.89.012311 |arxiv=1305.3955 |bibcode=2014PhRvA..89a2311H }}
• {{cite journal |last1=Hotta |first1=Masahiro |title=Quantum energy teleportation with trapped ions |journal=Physical Review A |date=22 October 2009 |volume=80 |issue=4 |page=042323 |doi=10.1103/PhysRevA.80.042323 |arxiv=0908.2824 |bibcode=2009PhRvA..80d2323H }}

• [https://www.quantamagazine.org/physicists-use-quantum-mechanics-to-pull-energy-out-of-nothing-20230222/ Physicists Use Quantum Mechanics to Pull Energy out of Nothing]
• [https://www.discovermagazine.com/the-sciences/first-demonstration-of-energy-teleportation First Demonstration of Energy Teleportation]
• [https://quantumfrontiers.com/2012/09/17/how-to-build-a-teleportation-machine-teleportation-protocol/ How to build a teleportation machine: Teleportation protocol]
• Introductory article about the protocol: {{arxiv|1101.3954}}
• [https://github.com/IKEDAKAZUKI/Quantum-Energy-Teleportation/blob/main/Quantum_Energy_Teleportation.ipynb Demonstration code of quantum energy teleportation using Qiskit is available in GitHub]

{{Quantum information }}

Category:Quantum information science

Category:Teleportation

Category:Vacuum