The Hamiltonian
H = J ∑⟨ij⟩ σi·σj + Jd ∑dimers σi·σj
Shastry-Sutherland lattice: a square lattice of bonds J with one diagonal bond Jd in every second plaquette, the orthogonal dimers. J = 0.8, Jd = 1, the couplings of the spin-1/2 form with S = σ/2, normalised to Jd = 1 (RULES.md 2.1); written here with Pauli matrices, so E/N in S units is E/(4N).
- lattice
- square
- sites
- 400
- boundary
- open
- J
- 0.8
- Jd
- 1
- energies
- 4
Stored as a total energy; quoted here as
E/N (S.S), which is what the papers report
(how the conversion works).
How these numbers were read
Where each number below was read, and how it was checked.
-0.442928(3), PEPS
Checked 2026-10-20 · source text of arXiv:2309.10955 read locally (arXiv HTML or pypdf layout text); value copied from the harvested cell and the text, no LLM transcription of numbers; first reading and an adversarial second reading (2026-10-20)
Reported as. -0.442928(3)
Table III, D = 10; version read: arXiv text (sources/2309.10955.txt); the journal version was not reached from this session, to be read on the verification pass (RULES.md 8) | Eq. (1) H = J1 sum S.S (square bonds) + J2 sum S.S (dimer bonds), Table III caption '20 x 20 SSM system at J1/J2 = 0.8 (set J2 = 1)'; per site: the section compares 'energy per site' of finite PEPS and iPEPS, and E_DVBS = -0.375. Table III does not say whether the average runs over the whole lattice or a central cluster; read as the whole lattice.
-0.442920(2), PEPS
Checked 2026-10-20 · source text of arXiv:2309.10955 read locally (arXiv HTML or pypdf layout text); value copied from the harvested cell and the text, no LLM transcription of numbers; first reading and an adversarial second reading (2026-10-20)
Reported as. -0.442920(2)
Table III, D = 8; version read: arXiv text (sources/2309.10955.txt); the journal version was not reached from this session, to be read on the verification pass (RULES.md 8) | Eq. (1) H = J1 sum S.S (square bonds) + J2 sum S.S (dimer bonds), Table III caption '20 x 20 SSM system at J1/J2 = 0.8 (set J2 = 1)'; per site: the section compares 'energy per site' of finite PEPS and iPEPS, and E_DVBS = -0.375. Table III does not say whether the average runs over the whole lattice or a central cluster; read as the whole lattice.
-0.442861(9), PEPS
Checked 2026-10-20 · source text of arXiv:2309.10955 read locally (arXiv HTML or pypdf layout text); value copied from the harvested cell and the text, no LLM transcription of numbers; first reading and an adversarial second reading (2026-10-20)
Reported as. -0.442861(9)
Table III, D = 6; version read: arXiv text (sources/2309.10955.txt); the journal version was not reached from this session, to be read on the verification pass (RULES.md 8) | Eq. (1) H = J1 sum S.S (square bonds) + J2 sum S.S (dimer bonds), Table III caption '20 x 20 SSM system at J1/J2 = 0.8 (set J2 = 1)'; per site: the section compares 'energy per site' of finite PEPS and iPEPS, and E_DVBS = -0.375. Table III does not say whether the average runs over the whole lattice or a central cluster; read as the whole lattice.
-0.442104(8), PEPS
Checked 2026-10-20 · source text of arXiv:2309.10955 read locally (arXiv HTML or pypdf layout text); value copied from the harvested cell and the text, no LLM transcription of numbers; first reading and an adversarial second reading (2026-10-20)
Reported as. -0.442104(8)
Table III, D = 4; version read: arXiv text (sources/2309.10955.txt); the journal version was not reached from this session, to be read on the verification pass (RULES.md 8) | Eq. (1) H = J1 sum S.S (square bonds) + J2 sum S.S (dimer bonds), Table III caption '20 x 20 SSM system at J1/J2 = 0.8 (set J2 = 1)'; per site: the section compares 'energy per site' of finite PEPS and iPEPS, and E_DVBS = -0.375. Table III does not say whether the average runs over the whole lattice or a central cluster; read as the whole lattice.