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 |
|---|---|---|---|---|---|---|---|---|---|
| 4747 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{6}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{5}M_{6}$ + ${ }M_{7}\phi_{1}q_{2}^{2}$ + ${ }M_{5}M_{8}$ | 0.7017 | 0.9024 | 0.7777 | [M:[0.8404, 0.8404, 0.891, 0.7899, 1.2101, 0.7899, 0.7394, 0.7899], q:[0.7394, 0.4202], qb:[0.3697, 0.7899], phi:[0.4202]] | [M:[[-4], [-4], [-9], [1], [-1], [1], [6], [1]], q:[[6], [-2]], qb:[[3], [1]], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{7}$, ${ }M_{4}$, ${ }M_{6}$, ${ }M_{8}$, ${ }M_{1}$, ${ }M_{2}$, ${ }\phi_{1}^{2}$, ${ }M_{3}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{7}^{2}$, ${ }M_{4}M_{7}$, ${ }M_{6}M_{7}$, ${ }M_{7}M_{8}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{4}^{2}$, ${ }M_{4}M_{6}$, ${ }M_{6}^{2}$, ${ }M_{1}M_{7}$, ${ }M_{2}M_{7}$, ${ }M_{4}M_{8}$, ${ }M_{6}M_{8}$, ${ }M_{8}^{2}$, ${ }M_{7}\phi_{1}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}M_{4}$, ${ }M_{2}M_{4}$, ${ }M_{1}M_{6}$, ${ }M_{2}M_{6}$, ${ }M_{3}M_{7}$, ${ }M_{1}M_{8}$, ${ }M_{2}M_{8}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{8}\phi_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{2}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{3}M_{6}$, ${ }M_{3}M_{8}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{2}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }M_{1}M_{3}$, ${ }M_{2}M_{3}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{3}^{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }M_{7}\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{6}\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{8}\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$ | ${}M_{1}\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}^{3}\tilde{q}_{1}^{2}$ | -1 | t^2.218 + 3*t^2.37 + 3*t^2.521 + t^2.673 + t^3.479 + t^4.436 + 5*t^4.588 + 10*t^4.739 + 9*t^4.891 + 8*t^5.043 + 3*t^5.194 + t^5.346 + 2*t^5.697 + 2*t^5.848 - t^6. - 3*t^6.152 - t^6.303 + t^6.654 + 5*t^6.806 + 13*t^6.957 + 21*t^7.109 + 22*t^7.261 + 21*t^7.412 + 17*t^7.564 + 8*t^7.716 + 3*t^7.867 + 2*t^7.915 + t^8.019 + 4*t^8.066 - 13*t^8.37 - 15*t^8.521 - 13*t^8.673 - 6*t^8.825 + t^8.872 - t^8.976 - t^4.261/y - t^6.479/y - (2*t^6.63)/y - (3*t^6.782)/y - t^6.934/y + (4*t^7.588)/y + (9*t^7.739)/y + (12*t^7.891)/y + (7*t^8.043)/y + (3*t^8.194)/y + t^8.848/y - t^4.261*y - t^6.479*y - 2*t^6.63*y - 3*t^6.782*y - t^6.934*y + 4*t^7.588*y + 9*t^7.739*y + 12*t^7.891*y + 7*t^8.043*y + 3*t^8.194*y + t^8.848*y | g1^6*t^2.218 + 3*g1*t^2.37 + (3*t^2.521)/g1^4 + t^2.673/g1^9 + g1^4*t^3.479 + g1^12*t^4.436 + 5*g1^7*t^4.588 + 10*g1^2*t^4.739 + (9*t^4.891)/g1^3 + (8*t^5.043)/g1^8 + (3*t^5.194)/g1^13 + t^5.346/g1^18 + 2*g1^10*t^5.697 + 2*g1^5*t^5.848 - t^6. - (3*t^6.152)/g1^5 - t^6.303/g1^10 + g1^18*t^6.654 + 5*g1^13*t^6.806 + 13*g1^8*t^6.957 + 21*g1^3*t^7.109 + (22*t^7.261)/g1^2 + (21*t^7.412)/g1^7 + (17*t^7.564)/g1^12 + (8*t^7.716)/g1^17 + (3*t^7.867)/g1^22 + 2*g1^16*t^7.915 + t^8.019/g1^27 + 4*g1^11*t^8.066 - 13*g1*t^8.37 - (15*t^8.521)/g1^4 - (13*t^8.673)/g1^9 - (6*t^8.825)/g1^14 + g1^24*t^8.872 - t^8.976/g1^19 - t^4.261/(g1^2*y) - (g1^4*t^6.479)/y - (2*t^6.63)/(g1*y) - (3*t^6.782)/(g1^6*y) - t^6.934/(g1^11*y) + (4*g1^7*t^7.588)/y + (9*g1^2*t^7.739)/y + (12*t^7.891)/(g1^3*y) + (7*t^8.043)/(g1^8*y) + (3*t^8.194)/(g1^13*y) + (g1^5*t^8.848)/y - (t^4.261*y)/g1^2 - g1^4*t^6.479*y - (2*t^6.63*y)/g1 - (3*t^6.782*y)/g1^6 - (t^6.934*y)/g1^11 + 4*g1^7*t^7.588*y + 9*g1^2*t^7.739*y + (12*t^7.891*y)/g1^3 + (7*t^8.043*y)/g1^8 + (3*t^8.194*y)/g1^13 + g1^5*t^8.848*y |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 2632 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{6}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{5}M_{6}$ + ${ }M_{7}\phi_{1}q_{2}^{2}$ | 0.6847 | 0.8722 | 0.785 | [M:[0.8384, 0.8384, 0.8864, 0.7904, 1.2096, 0.7904, 0.7424], q:[0.7424, 0.4192], qb:[0.3712, 0.7904], phi:[0.4192]] | t^2.227 + 2*t^2.371 + 3*t^2.515 + t^2.659 + t^3.485 + t^3.629 + t^4.454 + 4*t^4.598 + 7*t^4.742 + 6*t^4.886 + 7*t^5.03 + 3*t^5.174 + t^5.318 + 2*t^5.712 + 2*t^5.856 + t^6. - t^4.258/y - t^4.258*y | detail |