Abstract
Outside equilibrium, the definition of basic thermodynamic observables such as temperature and voltage are muddled by a competing panoply of “operation definitions” which are often contradictory. Here we define temperature and voltage on an equal footing by means of an equilibrium probe reservoir (such as an STM) coupled locally to the nonequilibrium system of interest; The temperature and voltage measurement are defined by requiring vanishing charge and heat dissipation into the probe. We show that temperature and voltage measurements are unique when they exist. We further derive a necessary and sufficient condition for the existence of a positive temperature solution. We then show that, when a positive temperature solution doesn’t exist, there must exist a negative temperature solution. The latter condition corresponds to a net population inversion. Therefore, a solution always exists. Our results suggest that a local temperature measurement without a simultaneous local voltage measurement, or vice-versa, is a misleading characterization of the state of the nonequilibrium system of interest. These results show an intimate connection to statements of the second law of thermodynamics. We see that the uniqueness of the (simultaneous) measurement of temperature and voltage is related to the Onsager’s statement of the second law of thermodynamics. Therefore, as an intermediate step, we provide the first proof for Onsager’s phenomenological statement (1931) for the case of quantum thermoelectric transport.
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- 1.
Voltage here refers to the electrochemical potential (μ) and not just the electrostatic potential (V). A voltmeter in fact measures the electrochemical potential difference which of course includes the electrostatic contribution μ = μ 0 + eV.
- 2.
- 3.
\(\mathcal {L}^{(\nu )}_{ps}(\mu _{p},T_{p})\) are finite even if \(\mathcal {T}_{ps}(\omega )\) and \(\omega \mathcal {T}_{ps}(\omega )\) do not obey the finite measure conditions of Postulate 2.1 due to the exponentially decaying tails of the Fermi-derivative. We merely need \(\mathcal {T}_{ps}(\omega )\) to grow slower than exponentially for ω →±∞.
- 4.
Furthermore, the tangent vector [see Eq. (2.34)] along \(I^{(1)}_{p}=c\) cannot be of magnitude zero since \(\mathcal {L}^{(2)}_{ps}\) is strictly positive for T p ∈ (0, ∞). Therefore, the contour \(I^{(1)}_{p}=c\) does not terminate for finite values of T p and μ p. This implies the existence of a function τ c : (−∞, ∞) → (0, ∞) which defines
$$\displaystyle \begin{aligned} T_{p}=\tau_{c}(\mu_{p}) \end{aligned}$$for each point on \(I^{(1)}_{p}(\mu _{p},T_{p})=c\).
- 5.
Transport in a vast majority of mesoscopic and nanoscale conductors are dominated by elastic processes at room temperature. Theorem 2.1 proves the Onsager’s phenomenological statement of the second law (1931) for quantum thermoelectric transport where elastic processes dominate the transport.
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Shastry, A. (2019). Temperature and Voltage. In: Theory of Thermodynamic Measurements of Quantum Systems Far from Equilibrium. Springer Theses. Springer, Cham. https://doi.org/10.1007/978-3-030-33574-8_2
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