Tropical-To-Toric Embedding Report
This page is a lightweight native-rendered mirror of the selected exact analysis artifact. Sage, Macaulay2, antichain selection, toric-ideal relations, and Miller-Sturmfels resolution data are computed before page generation; the browser only draws precomputed JSON and handles simple hover/click interactions.
No demo sidecars are accepted. The displayed staircase is derived from the checkpoint embedding payload through exact product-order antichain selection, then certified by Sage and Macaulay2.
Interactive Miller-Sturmfels Staircase
This native viewer draws the exact precomputed quotient-basis lattice points, minimal generators, adjacent LCM layer, and ideal region. The overhead mode shows the Miller-Sturmfels xy-grid; the projected 3D mode lifts module layers by small heights while keeping the same underlying exact lattice data.
record_000
| exponents | 7 |
|---|---|
| dimension | 2 |
| Sage normal fan exact | True |
| Macaulay2 toric ideal exact | True |
| selection | staircase_antichain |
| input unique checkpoint exponents | 435 |
| minimal generators | [[25, 0], [24, 6], [17, 27], [16, 30], [13, 32], [2, 34], [0, 48]] |
| quotient-basis lattice points | 791 |
| adjacent LCM corners | 6 |
| Macaulay2 toric ideal generators | 96 |
| Macaulay2 resolution length | 7 |
| Macaulay2 regularity | 35 |
summary JSONexact CAS sidecar JSON
Complete Macaulay2 toric ideal relation list (96)
x_1^2*x_5^2*x_6-x_4^4x_0*x_1*x_4*x_5*x_6-x_3^4x_2^2*x_5^4-x_3*x_4^2*x_6^2x_2^2*x_4^2*x_5^2-x_1^2*x_3*x_6^3x_0^3*x_3*x_5^2-x_1^2*x_2^2*x_4x_0*x_4^5-x_1*x_3^4*x_5x_0^3*x_3*x_4^3-x_1^4*x_2^2*x_6x_0*x_1^3*x_6^4-x_2^2*x_3^3*x_4*x_5x_0^3*x_3^2*x_6^3-x_2^4*x_4^3x_0^4*x_5^3*x_6-x_1*x_2^2*x_3^3x_0^3*x_4*x_5^4-x_1^4*x_6^3x_2^2*x_3^3*x_5^3-x_0*x_1*x_4^3*x_6^3x_1^4*x_3*x_5^3-x_0^2*x_2^4*x_6x_1^2*x_2^4*x_5^2-x_0^3*x_3^2*x_4*x_6^2x_1^2*x_3*x_4^4*x_5-x_0^2*x_2^4*x_6^2x_1^6*x_4*x_5-x_0^5*x_2^2*x_6x_0^2*x_3^5*x_5-x_1^3*x_2^2*x_4^2*x_6x_2^8-x_1*x_3^7x_0^4*x_4^2*x_6^3-x_1*x_2^4*x_3^2*x_5x_0^3*x_5^6-x_1^2*x_4^3*x_6^2x_1^2*x_4^2*x_5^5-x_0^2*x_2^2*x_6^4x_4^6*x_5^3-x_0^2*x_2^2*x_6^5x_0*x_3^2*x_4^3*x_5^3-x_2^6*x_6^2x_0^2*x_3^4*x_5^3-x_1^5*x_6^4x_0^4*x_4^4*x_5-x_1^3*x_2^2*x_3^3x_0^2*x_2^6*x_5-x_1^4*x_3^2*x_4^2*x_6x_0^4*x_1*x_5*x_6^4-x_2^4*x_3^2*x_4^2x_1^5*x_4^3*x_6^2-x_0*x_2^6*x_3^2x_0*x_3*x_4*x_5^7-x_2^4*x_6^4x_0*x_1^2*x_3^2*x_5^5-x_2^6*x_4*x_6x_1^5*x_4*x_5^4-x_0*x_2^4*x_3^3x_1^4*x_4^3*x_5^3-x_0^5*x_3*x_6^4x_1^3*x_4^5*x_5^2-x_0*x_2^4*x_3^3*x_6x_3^6*x_4^2*x_5^2-x_1*x_2^6*x_6^3x_1*x_2^4*x_4^4*x_5-x_0^2*x_3^6*x_6^2x_1*x_4^9-x_0*x_2^4*x_3^3*x_6^2x_0^4*x_1*x_6^6-x_2^6*x_3*x_5^3x_0^6*x_6^5-x_1^3*x_3^3*x_4^2*x_5^2x_1^6*x_3^2*x_5*x_6^2-x_0^2*x_2^6*x_4^2x_0^6*x_3^3*x_6^2-x_1^4*x_2^6x_0^8*x_3*x_5*x_6-x_1^8*x_4^2x_1^2*x_5^9-x_0^2*x_3*x_6^6x_4^4*x_5^7-x_0^2*x_3*x_6^7x_1^4*x_5^7-x_0^2*x_2^2*x_4^2*x_6^3x_3^5*x_5^6-x_1*x_2^4*x_6^5x_0^2*x_1^3*x_5^6-x_2^6*x_3^2x_1^6*x_5^5-x_0^5*x_3*x_4*x_6^3x_0^2*x_1*x_4^4*x_5^4-x_2^6*x_3^2*x_6x_1^8*x_5^3-x_0^5*x_2^2*x_4^3x_0*x_2^6*x_3^2*x_5^2-x_1^3*x_4^7*x_6x_0^5*x_2^4*x_4*x_5-x_1^8*x_3*x_6^2x_1^5*x_4^6-x_0^4*x_2^2*x_3^4*x_6x_0^8*x_3*x_4^2-x_1^10*x_5x_0^7*x_4*x_5*x_6^3-x_1^3*x_2^6*x_3x_1^9*x_6^3-x_0^4*x_2^4*x_3^3x_0*x_5^11-x_2^2*x_4*x_6^6x_1*x_3^3*x_5^8-x_0^3*x_4*x_6^7x_3^3*x_4^3*x_5^6-x_0^3*x_1*x_6^8x_0^5*x_2^4*x_5^3-x_1^6*x_3*x_4^3*x_6x_0*x_3^9*x_5^2-x_1^2*x_2^2*x_4^7*x_6x_0^3*x_2^6*x_4^3-x_1^5*x_3^6*x_6x_0^7*x_3^5-x_1^9*x_4^3x_0^9*x_5^2*x_6^2-x_1^7*x_3^3*x_4x_0^9*x_4^3*x_6-x_1^9*x_3^3x_0*x_4^3*x_5^9-x_1^2*x_2^2*x_6^7x_0^2*x_1*x_4^2*x_5^8-x_2^4*x_3^3*x_6^3x_3^5*x_4^4*x_5^4-x_1^3*x_2^4*x_6^6x_0*x_3^8*x_5^4-x_1^4*x_4^5*x_6^4x_0^7*x_4^3*x_5^3-x_1^5*x_2^4*x_3^2x_3^10*x_5^3-x_0*x_2^6*x_4^3*x_6^3x_0^8*x_2^2*x_5^3-x_1^10*x_6^2x_4^11*x_5^2-x_0*x_1*x_2^2*x_3^4*x_6^5x_1^5*x_2^6*x_4*x_5-x_0^5*x_3^7*x_6x_2^4*x_4^9-x_0*x_3^10*x_6^2x_0^9*x_4*x_6^4-x_1^7*x_2^2*x_3^2*x_5^2x_3^4*x_5^10-x_1*x_2^2*x_4^2*x_6^7x_3^4*x_4^2*x_5^8-x_1^3*x_2^2*x_6^8x_3^9*x_5^5-x_0*x_1^2*x_2^4*x_4*x_6^6x_4^14-x_2^4*x_3^7*x_5*x_6^2x_3^3*x_5^12-x_1^3*x_6^10x_0^11*x_3^2*x_4*x_5-x_1^12*x_2^2x_0^12*x_6^4-x_1^9*x_2^4*x_3x_1^4*x_2^6*x_4^6-x_0^4*x_3^11*x_6x_0^10*x_2^6-x_1^14*x_3*x_6x_0^12*x_4^2*x_5^2*x_6-x_1^11*x_2^2*x_3^2x_0^16*x_3^2*x_6-x_1^18x_0^13*x_2^4*x_5^2-x_1^16*x_4*x_6x_0^13*x_2^4*x_4^3-x_1^18*x_6^2x_0^17*x_4*x_5*x_6^2-x_1^17*x_3^2x_4^3*x_5^18-x_0*x_2^2*x_3*x_6^13x_1*x_3^2*x_4^3*x_5^15-x_0^5*x_6^14x_0^12*x_2^4*x_3^4*x_5-x_1^17*x_4^2*x_6^2x_4*x_5^22-x_0*x_3^2*x_6^15x_3^2*x_5^21-x_0^2*x_1*x_6^16x_1*x_3*x_5^30-x_0^4*x_6^22x_5^33-x_2^2*x_3^2*x_6^21
Miller-Sturmfels S/I Resolution
| basis | LCM shift | differential | d1 d2 check |
|---|---|---|---|
| f_0 | x^25 y^6 | d2(f_0) = y^6 e_0 - x e_1 | d1 d2(f_0) = x^25 y^6 - x^25 y^6 = 0 |
| f_1 | x^24 y^27 | d2(f_1) = y^21 e_1 - x^7 e_2 | d1 d2(f_1) = x^24 y^27 - x^24 y^27 = 0 |
| f_2 | x^17 y^30 | d2(f_2) = y^3 e_2 - x e_3 | d1 d2(f_2) = x^17 y^30 - x^17 y^30 = 0 |
| f_3 | x^16 y^32 | d2(f_3) = y^2 e_3 - x^3 e_4 | d1 d2(f_3) = x^16 y^32 - x^16 y^32 = 0 |
| f_4 | x^13 y^34 | d2(f_4) = y^2 e_4 - x^11 e_5 | d1 d2(f_4) = x^13 y^34 - x^13 y^34 = 0 |
| f_5 | x^2 y^48 | d2(f_5) = y^14 e_5 - x^2 e_6 | d1 d2(f_5) = x^2 y^48 - x^2 y^48 = 0 |