# Spin-charge split pairing in underdoped cuprate superconductors: support from low-$T$ specific heat

## TL;DR

This paper models the specific heat of underdoped cuprates, supporting the split-pairing mechanism where spinons and holons pair separately before Bose condensation, explaining experimental specific heat data.

## Contribution

It provides a theoretical calculation of specific heat consistent with experiments, supporting the split-pairing mechanism in underdoped cuprates.

## Key findings

- Calculated specific heat matches experimental data.
- Supports split-pairing of spinons and holons.
- Explains the T-linear and T^3 terms in specific heat.

## Abstract

We calculate the specific heat of a weakly interacting dilute system of bosons on a lattice and show that it is consistent with the measured electronic specific heat in the superconducting state of underdoped cuprates with boson concentration $\rho \sim x/2$, where $x$ is the hole (dopant) concentration. As usual, the $T^3$ term is due to Goldstone phonons. The zero-point energy, through its dependence on the condensate density $\rho_0(T)$, accounts for the anomalous $T$-linear term. These results support the split-pairing mechanism, in which spinons (pure spin) are paired at $T^*$ and holons (pure charge) form real-space pairs at $T_p < T^*$, creating a gauge-coupled physical pair of charge $+2e$ and concentration $x/2$ which Bose condenses below $T_c$, accounting for the observed phases.