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 |
|---|---|---|---|---|---|---|---|---|---|
| 50805 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{3}M_{4}$ + ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$ + ${ }M_{5}q_{1}\tilde{q}_{2}$ + ${ }M_{2}^{2}$ + ${ }M_{3}M_{6}$ | 0.7136 | 0.8827 | 0.8085 | [M:[0.8177, 1.0, 1.0912, 0.9088, 0.9544, 0.9088], q:[0.5684, 0.614], qb:[0.4316, 0.4772], phi:[0.4772]] | [M:[[8], [0], [-4], [4], [2], [4]], q:[[-3], [-5]], qb:[[3], [1]], phi:[[1]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{1}$, ${ }M_{4}$, ${ }M_{6}$, ${ }M_{5}$, ${ }\phi_{1}^{2}$, ${ }M_{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }M_{1}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{1}M_{4}$, ${ }M_{1}M_{6}$, ${ }M_{1}M_{5}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{4}^{2}$, ${ }M_{4}M_{6}$, ${ }M_{6}^{2}$, ${ }M_{4}M_{5}$, ${ }M_{5}M_{6}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{2}M_{4}$, ${ }M_{5}^{2}$, ${ }M_{2}M_{6}$, ${ }M_{5}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }M_{2}M_{5}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{4}q_{2}\tilde{q}_{1}$, ${ }M_{6}q_{2}\tilde{q}_{1}$ | ${}M_{5}q_{2}\tilde{q}_{1}$ | -1 | t^2.453 + 2*t^2.727 + 2*t^2.863 + t^3. + t^3.137 + t^4.021 + t^4.158 + t^4.295 + t^4.432 + 2*t^4.568 + t^4.705 + t^4.842 + t^4.906 + t^4.979 + t^5.115 + 2*t^5.18 + 2*t^5.316 + 3*t^5.453 + 3*t^5.59 + 4*t^5.727 + 2*t^5.863 - t^6. - t^6.137 - t^6.273 - 2*t^6.41 + t^6.474 - t^6.547 + t^6.611 + 3*t^6.748 + 4*t^6.885 + 5*t^7.021 + 4*t^7.158 + 4*t^7.295 + t^7.359 + 4*t^7.432 + 3*t^7.568 + 2*t^7.633 + t^7.705 + 2*t^7.769 + t^7.842 + 3*t^7.906 + t^7.979 + 4*t^8.043 - t^8.115 + 7*t^8.18 - t^8.252 + 4*t^8.316 + 4*t^8.453 + 6*t^8.59 - 3*t^8.727 - 4*t^8.863 + t^8.927 - t^4.432/y - t^6.885/y - t^7.158/y - (2*t^7.295)/y + (2*t^7.568)/y + t^7.705/y + t^7.979/y + (2*t^8.18)/y + (2*t^8.316)/y + (2*t^8.453)/y + (5*t^8.59)/y + (3*t^8.727)/y + (4*t^8.863)/y - t^4.432*y - t^6.885*y - t^7.158*y - 2*t^7.295*y + 2*t^7.568*y + t^7.705*y + t^7.979*y + 2*t^8.18*y + 2*t^8.316*y + 2*t^8.453*y + 5*t^8.59*y + 3*t^8.727*y + 4*t^8.863*y | g1^8*t^2.453 + 2*g1^4*t^2.727 + 2*g1^2*t^2.863 + t^3. + t^3.137/g1^2 + g1^7*t^4.021 + g1^5*t^4.158 + g1^3*t^4.295 + g1*t^4.432 + (2*t^4.568)/g1 + t^4.705/g1^3 + t^4.842/g1^5 + g1^16*t^4.906 + t^4.979/g1^7 + t^5.115/g1^9 + 2*g1^12*t^5.18 + 2*g1^10*t^5.316 + 3*g1^8*t^5.453 + 3*g1^6*t^5.59 + 4*g1^4*t^5.727 + 2*g1^2*t^5.863 - t^6. - t^6.137/g1^2 - t^6.273/g1^4 - (2*t^6.41)/g1^6 + g1^15*t^6.474 - t^6.547/g1^8 + g1^13*t^6.611 + 3*g1^11*t^6.748 + 4*g1^9*t^6.885 + 5*g1^7*t^7.021 + 4*g1^5*t^7.158 + 4*g1^3*t^7.295 + g1^24*t^7.359 + 4*g1*t^7.432 + (3*t^7.568)/g1 + 2*g1^20*t^7.633 + t^7.705/g1^3 + 2*g1^18*t^7.769 + t^7.842/g1^5 + 3*g1^16*t^7.906 + t^7.979/g1^7 + 4*g1^14*t^8.043 - t^8.115/g1^9 + 7*g1^12*t^8.18 - t^8.252/g1^11 + 4*g1^10*t^8.316 + 4*g1^8*t^8.453 + 6*g1^6*t^8.59 - 3*g1^4*t^8.727 - 4*g1^2*t^8.863 + g1^23*t^8.927 - (g1*t^4.432)/y - (g1^9*t^6.885)/y - (g1^5*t^7.158)/y - (2*g1^3*t^7.295)/y + (2*t^7.568)/(g1*y) + t^7.705/(g1^3*y) + t^7.979/(g1^7*y) + (2*g1^12*t^8.18)/y + (2*g1^10*t^8.316)/y + (2*g1^8*t^8.453)/y + (5*g1^6*t^8.59)/y + (3*g1^4*t^8.727)/y + (4*g1^2*t^8.863)/y - g1*t^4.432*y - g1^9*t^6.885*y - g1^5*t^7.158*y - 2*g1^3*t^7.295*y + (2*t^7.568*y)/g1 + (t^7.705*y)/g1^3 + (t^7.979*y)/g1^7 + 2*g1^12*t^8.18*y + 2*g1^10*t^8.316*y + 2*g1^8*t^8.453*y + 5*g1^6*t^8.59*y + 3*g1^4*t^8.727*y + 4*g1^2*t^8.863*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 |
|---|---|---|---|---|---|---|---|---|---|
| 47067 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{3}M_{4}$ + ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$ + ${ }M_{5}q_{1}\tilde{q}_{2}$ + ${ }M_{2}^{2}$ | 0.706 | 0.8681 | 0.8132 | [M:[0.8498, 1.0, 1.0751, 0.9249, 0.9624], q:[0.5563, 0.5939], qb:[0.4437, 0.4812], phi:[0.4812]] | t^2.549 + t^2.775 + 2*t^2.887 + t^3. + t^3.113 + t^3.225 + t^4.106 + t^4.218 + t^4.331 + t^4.444 + 2*t^4.556 + t^4.669 + t^4.782 + t^4.894 + t^5.007 + t^5.099 + t^5.324 + 2*t^5.437 + t^5.549 + t^5.662 + 4*t^5.775 + t^5.887 - t^4.444/y - t^4.444*y | detail |