{"inputSchema":{"type":"object","additionalProperties":false,"required":["artifact"],"properties":{"artifact":{"type":"object","additionalProperties":false,"required":["dicke"],"properties":{"dicke":{"type":"object","additionalProperties":false,"required":["data","claim"],"properties":{"data":{"type":"object","additionalProperties":false,"required":["atom_count","maximum_boson_number","boson_frequency","atomic_frequency","coupling","inverse_temperature"],"properties":{"atom_count":{"type":"integer","minimum":1,"maximum":3},"maximum_boson_number":{"type":"integer","minimum":1,"maximum":5},"boson_frequency":{"type":"number","minimum":0.5,"maximum":2},"atomic_frequency":{"type":"number","minimum":0.5,"maximum":2},"coupling":{"type":"number","minimum":0,"maximum":1},"inverse_temperature":{"type":"number","minimum":0.2,"maximum":2}}},"claim":{}}}}}}},"method":"POST","url":"https://detect.halowerk.com/v1/F-TD2000-GEO-INDUSTRY-B023/finite-dicke-light-matter-parity-spectrum-thermal-occupation-law"}