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 |
|---|---|---|---|---|---|---|---|---|---|
| 47178 | SU2adj1nf2 | ${}\phi_{1}q_{1}q_{2}$ + ${ }M_{1}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{2}\tilde{q}_{1}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{3}$ + ${ }M_{3}\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{4}q_{1}\tilde{q}_{1}$ + ${ }M_{5}\phi_{1}\tilde{q}_{1}^{2}$ | 0.5745 | 0.7465 | 0.7697 | [M:[0.8498, 1.1502, 0.7253, 0.674, 0.9744], q:[1.0256, 0.5495], qb:[0.3004, 0.4249], phi:[0.4249]] | [M:[[2], [-2], [-3], [11], [7]], q:[[-7], [6]], qb:[[-4], [1]], phi:[[1]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{4}$, ${ }M_{3}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}$, ${ }\phi_{1}^{2}$, ${ }M_{5}$, ${ }q_{2}\tilde{q}_{2}$, ${ }M_{2}$, ${ }M_{4}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{4}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\tilde{q}_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}M_{4}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{1}M_{3}$, ${ }M_{3}\phi_{1}^{2}$, ${ }q_{1}q_{2}$, ${ }M_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{4}M_{5}$, ${ }M_{4}q_{2}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }M_{3}M_{5}$, ${ }M_{1}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }M_{3}q_{2}\tilde{q}_{2}$, ${ }M_{5}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }M_{2}M_{4}$, ${ }M_{1}M_{5}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{1}q_{2}\tilde{q}_{2}$, ${ }M_{2}M_{3}$, ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{5}^{2}$, ${ }M_{5}q_{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$ | ${}M_{1}M_{2}$ | -2 | t^2.022 + 2*t^2.176 + 2*t^2.549 + 2*t^2.923 + t^3.451 + t^4.044 + 2*t^4.198 + 4*t^4.352 + 2*t^4.572 + 5*t^4.725 + 2*t^4.945 + 6*t^5.099 + 4*t^5.473 + t^5.626 + 3*t^5.846 - 2*t^6. + t^6.066 + 2*t^6.22 + 3*t^6.374 + 4*t^6.527 + 2*t^6.594 + 4*t^6.747 + 6*t^6.901 + 2*t^6.967 + 6*t^7.121 + 10*t^7.275 - t^7.428 + 4*t^7.495 + 9*t^7.648 - t^7.802 + 3*t^7.868 + 6*t^8.022 + t^8.088 - 8*t^8.176 + 2*t^8.242 + 7*t^8.396 - 4*t^8.549 + 2*t^8.616 + 4*t^8.703 + 8*t^8.769 - 4*t^8.923 + 2*t^8.989 - t^4.275/y - t^6.297/y - t^6.451/y - t^6.824/y + t^7.198/y + (2*t^7.352)/y + (2*t^7.572)/y + (5*t^7.725)/y + (2*t^7.945)/y + (6*t^8.099)/y + t^8.253/y - t^8.319/y + (4*t^8.473)/y + t^8.626/y - t^4.275*y - t^6.297*y - t^6.451*y - t^6.824*y + t^7.198*y + 2*t^7.352*y + 2*t^7.572*y + 5*t^7.725*y + 2*t^7.945*y + 6*t^8.099*y + t^8.253*y - t^8.319*y + 4*t^8.473*y + t^8.626*y | g1^11*t^2.022 + (2*t^2.176)/g1^3 + 2*g1^2*t^2.549 + 2*g1^7*t^2.923 + t^3.451/g1^2 + g1^22*t^4.044 + 2*g1^8*t^4.198 + (4*t^4.352)/g1^6 + 2*g1^13*t^4.572 + (5*t^4.725)/g1 + 2*g1^18*t^4.945 + 6*g1^4*t^5.099 + 4*g1^9*t^5.473 + t^5.626/g1^5 + 3*g1^14*t^5.846 - 2*t^6. + g1^33*t^6.066 + 2*g1^19*t^6.22 + 3*g1^5*t^6.374 + (4*t^6.527)/g1^9 + 2*g1^24*t^6.594 + 4*g1^10*t^6.747 + (6*t^6.901)/g1^4 + 2*g1^29*t^6.967 + 6*g1^15*t^7.121 + 10*g1*t^7.275 - t^7.428/g1^13 + 4*g1^20*t^7.495 + 9*g1^6*t^7.648 - t^7.802/g1^8 + 3*g1^25*t^7.868 + 6*g1^11*t^8.022 + g1^44*t^8.088 - (8*t^8.176)/g1^3 + 2*g1^30*t^8.242 + 7*g1^16*t^8.396 - 4*g1^2*t^8.549 + 2*g1^35*t^8.616 + (4*t^8.703)/g1^12 + 8*g1^21*t^8.769 - 4*g1^7*t^8.923 + 2*g1^40*t^8.989 - (g1*t^4.275)/y - (g1^12*t^6.297)/y - t^6.451/(g1^2*y) - (g1^3*t^6.824)/y + (g1^8*t^7.198)/y + (2*t^7.352)/(g1^6*y) + (2*g1^13*t^7.572)/y + (5*t^7.725)/(g1*y) + (2*g1^18*t^7.945)/y + (6*g1^4*t^8.099)/y + t^8.253/(g1^10*y) - (g1^23*t^8.319)/y + (4*g1^9*t^8.473)/y + t^8.626/(g1^5*y) - g1*t^4.275*y - g1^12*t^6.297*y - (t^6.451*y)/g1^2 - g1^3*t^6.824*y + g1^8*t^7.198*y + (2*t^7.352*y)/g1^6 + 2*g1^13*t^7.572*y + (5*t^7.725*y)/g1 + 2*g1^18*t^7.945*y + 6*g1^4*t^8.099*y + (t^8.253*y)/g1^10 - g1^23*t^8.319*y + 4*g1^9*t^8.473*y + (t^8.626*y)/g1^5 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 46551 | SU2adj1nf2 | ${}\phi_{1}q_{1}q_{2}$ + ${ }M_{1}\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}q_{2}\tilde{q}_{1}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{3}$ + ${ }M_{3}\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{4}q_{1}\tilde{q}_{1}$ | 0.5734 | 0.743 | 0.7718 | [M:[0.8579, 1.1421, 0.7131, 0.7187], q:[0.9972, 0.5738], qb:[0.2841, 0.429], phi:[0.429]] | 2*t^2.139 + t^2.156 + 2*t^2.574 + t^2.992 + t^3.008 + t^3.426 + 4*t^4.279 + 2*t^4.295 + t^4.312 + 5*t^4.713 + 2*t^4.73 + 2*t^5.131 + 5*t^5.148 + t^5.164 + 3*t^5.565 + 2*t^5.582 + t^5.983 - t^6. - t^4.287/y - t^4.287*y | detail |