Chosen Fixed Point
Here is the data for the chosen fixed point.
$F_{UV}$ represents the flavor symmetries in the UV Lagrangian, and $F_{IR}$ represents the flavor symmetries in the IR. $F_{UV}$ and $F_{IR}$ can differ due to accidental symmetry enhancement.
The number of marginal operators, $n_{marginal}$, minus the dimension of flavor symmetries in IR, $|F_{IR}|$, corresponds to the coefficient of $t^6$ in the superconformal index.
| # | Theory | Superpotential | Central charge $a$ | Central charge $c$ | Ratio $a/c$ | Matter field: $R$-charge | U(1) part of $F_{UV}$ | Rank of $F_{UV}$ | Rational |
|---|---|---|---|---|---|---|---|---|---|
| 2537 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{2}M_{3}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{6}q_{1}\tilde{q}_{2}$ + ${ }M_{1}M_{7}$ | 0.6961 | 0.8551 | 0.814 | [M:[1.0099, 0.9703, 1.0297, 0.9505, 1.0495, 0.9307, 0.9901], q:[0.505, 0.4851], qb:[0.4653, 0.5644], phi:[0.495]] | [M:[[2], [-6], [6], [-10], [10], [-14], [-2]], q:[[1], [-3]], qb:[[-7], [13]], phi:[[-1]]] | {a: 113613/163216, c: 69785/81608, M1: 102/101, M2: 98/101, M3: 104/101, M4: 96/101, M5: 106/101, M6: 94/101, M7: 100/101, q1: 51/101, q2: 49/101, qb1: 47/101, qb2: 57/101, phi1: 50/101} |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{6}$, ${ }M_{4}$, ${ }M_{2}$, ${ }M_{7}$, ${ }\phi_{1}^{2}$, ${ }M_{3}$, ${ }M_{5}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{6}^{2}$, ${ }M_{4}M_{6}$, ${ }M_{4}^{2}$, ${ }M_{2}M_{6}$, ${ }M_{2}M_{4}$, ${ }M_{6}M_{7}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{2}^{2}$, ${ }M_{4}M_{7}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{3}M_{6}$, ${ }M_{2}M_{7}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{5}M_{6}$, ${ }M_{7}^{2}$, ${ }M_{7}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$ | ${}$ | -2 | t^2.792 + t^2.851 + t^2.911 + 2*t^2.97 + t^3.089 + t^3.149 + t^4.277 + t^4.337 + 2*t^4.396 + t^4.455 + t^4.515 + t^4.574 + t^4.634 + t^4.693 + t^4.871 + t^5.584 + t^5.644 + t^5.703 + 2*t^5.762 + 2*t^5.822 + 2*t^5.881 + 3*t^5.941 - 2*t^6. + t^6.119 + t^7.069 + 2*t^7.129 + 3*t^7.188 + 4*t^7.248 + 3*t^7.307 + 5*t^7.366 + 2*t^7.426 + 2*t^7.485 + t^7.545 + t^7.604 + 2*t^7.663 + t^7.782 + 2*t^7.842 - t^7.901 + t^7.96 + t^8.02 + t^8.376 + t^8.436 + t^8.495 + 3*t^8.554 + 3*t^8.614 + 4*t^8.673 + 4*t^8.733 + 2*t^8.792 + t^8.911 - 4*t^8.97 - t^4.485/y - t^7.277/y - t^7.455/y + t^7.515/y + t^7.693/y + t^8.644/y + t^8.703/y + (3*t^8.762)/y + (2*t^8.822)/y + (3*t^8.881)/y + (3*t^8.941)/y - t^4.485*y - t^7.277*y - t^7.455*y + t^7.515*y + t^7.693*y + t^8.644*y + t^8.703*y + 3*t^8.762*y + 2*t^8.822*y + 3*t^8.881*y + 3*t^8.941*y | t^2.792/g1^14 + t^2.851/g1^10 + t^2.911/g1^6 + (2*t^2.97)/g1^2 + g1^6*t^3.089 + g1^10*t^3.149 + t^4.277/g1^15 + t^4.337/g1^11 + (2*t^4.396)/g1^7 + t^4.455/g1^3 + g1*t^4.515 + g1^5*t^4.574 + g1^9*t^4.634 + g1^13*t^4.693 + g1^25*t^4.871 + t^5.584/g1^28 + t^5.644/g1^24 + t^5.703/g1^20 + (2*t^5.762)/g1^16 + (2*t^5.822)/g1^12 + (2*t^5.881)/g1^8 + (3*t^5.941)/g1^4 - 2*t^6. + g1^8*t^6.119 + t^7.069/g1^29 + (2*t^7.129)/g1^25 + (3*t^7.188)/g1^21 + (4*t^7.248)/g1^17 + (3*t^7.307)/g1^13 + (5*t^7.366)/g1^9 + (2*t^7.426)/g1^5 + (2*t^7.485)/g1 + g1^3*t^7.545 + g1^7*t^7.604 + 2*g1^11*t^7.663 + g1^19*t^7.782 + 2*g1^23*t^7.842 - g1^27*t^7.901 + g1^31*t^7.96 + g1^35*t^8.02 + t^8.376/g1^42 + t^8.436/g1^38 + t^8.495/g1^34 + (3*t^8.554)/g1^30 + (3*t^8.614)/g1^26 + (4*t^8.673)/g1^22 + (4*t^8.733)/g1^18 + (2*t^8.792)/g1^14 + t^8.911/g1^6 - (4*t^8.97)/g1^2 - t^4.485/(g1*y) - t^7.277/(g1^15*y) - t^7.455/(g1^3*y) + (g1*t^7.515)/y + (g1^13*t^7.693)/y + t^8.644/(g1^24*y) + t^8.703/(g1^20*y) + (3*t^8.762)/(g1^16*y) + (2*t^8.822)/(g1^12*y) + (3*t^8.881)/(g1^8*y) + (3*t^8.941)/(g1^4*y) - (t^4.485*y)/g1 - (t^7.277*y)/g1^15 - (t^7.455*y)/g1^3 + g1*t^7.515*y + g1^13*t^7.693*y + (t^8.644*y)/g1^24 + (t^8.703*y)/g1^20 + (3*t^8.762*y)/g1^16 + (2*t^8.822*y)/g1^12 + (3*t^8.881*y)/g1^8 + (3*t^8.941*y)/g1^4 |
Deformation
Here is the data for the deformed fixed points from the chosen fixed point.
| # | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
|---|
Equivalent Fixed Points from Other Seed Theories
Here is a list of equivalent fixed points from other gauge theories.
| # | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
|---|
Equivalent Fixed Points from the Same Seed Theory
Below is a list of equivalent fixed points from the same seed theories.
| id | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | More Info. | Rational |
|---|
Previous Theory
The previous fixed point before deforming to get the chosen fixed point.
| # | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
|---|---|---|---|---|---|---|---|---|---|
| 1443 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{2}M_{3}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{6}q_{1}\tilde{q}_{2}$ | 0.6952 | 0.8534 | 0.8146 | [M:[1.0089, 0.9733, 1.0267, 0.9554, 1.0446, 0.9376], q:[0.5045, 0.4866], qb:[0.4688, 0.5579], phi:[0.4955]] | t^2.813 + t^2.866 + t^2.92 + t^2.973 + t^3.027 + t^3.08 + t^3.134 + t^4.299 + t^4.353 + 2*t^4.406 + t^4.46 + t^4.513 + t^4.567 + t^4.62 + t^4.674 + t^4.834 + t^5.626 + t^5.679 + t^5.733 + t^5.786 + 2*t^5.84 + 2*t^5.893 + 2*t^5.947 - t^6. - t^4.487/y - t^4.487*y | detail |