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 |
|---|---|---|---|---|---|---|---|---|---|
| 1943 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }\phi_{1}\tilde{q}_{1}^{2}$ | 0.6055 | 0.7763 | 0.78 | [M:[1.0233, 0.9922, 0.7714, 1.2442, 0.7558], q:[0.4806, 0.4961], qb:[0.7481, 0.2597], phi:[0.5039]] | [M:[[12], [-4], [11], [-3], [3]], q:[[-10], [-2]], qb:[[-1], [5]], phi:[[2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}q_{1}\tilde{q}_{2}$, ${ }M_{5}$, ${ }M_{3}$, ${ }M_{2}$, ${ }\phi_{1}^{2}$, ${ }M_{1}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{4}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{5}q_{1}\tilde{q}_{2}$, ${ }M_{5}^{2}$, ${ }M_{3}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}M_{5}$, ${ }M_{3}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{2}M_{5}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }M_{2}M_{3}$, ${ }M_{5}\phi_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}^{3}$, ${ }M_{1}M_{5}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{1}M_{3}$, ${ }M_{3}\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{2}^{2}$, ${ }M_{4}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}\tilde{q}_{2}^{2}$ | ${}M_{5}\phi_{1}q_{1}\tilde{q}_{2}$ | 0 | t^2.221 + t^2.267 + t^2.314 + t^2.977 + t^3.023 + 2*t^3.07 + 2*t^3.733 + t^3.779 + t^4.395 + 2*t^4.442 + 2*t^4.488 + 2*t^4.535 + t^4.582 + t^4.628 + t^5.198 + 2*t^5.244 + 3*t^5.291 + 2*t^5.337 + 2*t^5.384 + t^5.953 + 3*t^6.047 + 3*t^6.093 + 3*t^6.14 + t^6.616 + t^6.663 + 2*t^6.709 + 3*t^6.756 + 5*t^6.802 + 3*t^6.849 + t^6.896 + t^6.942 + t^7.418 + 3*t^7.465 + 4*t^7.512 + 4*t^7.558 + 4*t^7.605 + 2*t^7.651 + 2*t^7.698 + t^8.128 - t^8.221 + t^8.267 + t^8.314 + 5*t^8.361 + 4*t^8.407 + 3*t^8.454 + t^8.79 + 2*t^8.837 + 2*t^8.883 + t^8.93 - t^8.977 - t^4.512/y - t^6.826/y + t^7.442/y + t^7.488/y + t^7.535/y + (2*t^8.198)/y + (2*t^8.244)/y + (4*t^8.291)/y + (3*t^8.337)/y + (2*t^8.384)/y + (2*t^8.953)/y - t^4.512*y - t^6.826*y + t^7.442*y + t^7.488*y + t^7.535*y + 2*t^8.198*y + 2*t^8.244*y + 4*t^8.291*y + 3*t^8.337*y + 2*t^8.384*y + 2*t^8.953*y | t^2.221/g1^5 + g1^3*t^2.267 + g1^11*t^2.314 + t^2.977/g1^4 + g1^4*t^3.023 + 2*g1^12*t^3.07 + (2*t^3.733)/g1^3 + g1^5*t^3.779 + t^4.395/g1^18 + (2*t^4.442)/g1^10 + (2*t^4.488)/g1^2 + 2*g1^6*t^4.535 + g1^14*t^4.582 + g1^22*t^4.628 + t^5.198/g1^9 + (2*t^5.244)/g1 + 3*g1^7*t^5.291 + 2*g1^15*t^5.337 + 2*g1^23*t^5.384 + t^5.953/g1^8 + 3*g1^8*t^6.047 + 3*g1^16*t^6.093 + 3*g1^24*t^6.14 + t^6.616/g1^23 + t^6.663/g1^15 + (2*t^6.709)/g1^7 + 3*g1*t^6.756 + 5*g1^9*t^6.802 + 3*g1^17*t^6.849 + g1^25*t^6.896 + g1^33*t^6.942 + t^7.418/g1^14 + (3*t^7.465)/g1^6 + 4*g1^2*t^7.512 + 4*g1^10*t^7.558 + 4*g1^18*t^7.605 + 2*g1^26*t^7.651 + 2*g1^34*t^7.698 + t^8.128/g1^21 - t^8.221/g1^5 + g1^3*t^8.267 + g1^11*t^8.314 + 5*g1^19*t^8.361 + 4*g1^27*t^8.407 + 3*g1^35*t^8.454 + t^8.79/g1^36 + (2*t^8.837)/g1^28 + (2*t^8.883)/g1^20 + t^8.93/g1^12 - t^8.977/g1^4 - (g1^2*t^4.512)/y - (g1^13*t^6.826)/y + t^7.442/(g1^10*y) + t^7.488/(g1^2*y) + (g1^6*t^7.535)/y + (2*t^8.198)/(g1^9*y) + (2*t^8.244)/(g1*y) + (4*g1^7*t^8.291)/y + (3*g1^15*t^8.337)/y + (2*g1^23*t^8.384)/y + (2*t^8.953)/(g1^8*y) - g1^2*t^4.512*y - g1^13*t^6.826*y + (t^7.442*y)/g1^10 + (t^7.488*y)/g1^2 + g1^6*t^7.535*y + (2*t^8.198*y)/g1^9 + (2*t^8.244*y)/g1 + 4*g1^7*t^8.291*y + 3*g1^15*t^8.337*y + 2*g1^23*t^8.384*y + (2*t^8.953*y)/g1^8 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 600 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{2}\phi_{1}^{2}$ | 0.7101 | 0.8727 | 0.8137 | [M:[0.8432, 1.0523, 0.8729, 1.0226, 0.9774], q:[0.6307, 0.5261], qb:[0.4964, 0.4513], phi:[0.4739]] | t^2.53 + t^2.619 + t^2.843 + t^2.932 + t^3.068 + t^3.157 + t^3.246 + t^4.129 + t^4.265 + t^4.354 + t^4.4 + t^4.489 + t^4.578 + t^4.668 + t^4.803 + t^4.892 + t^5.059 + t^5.148 + t^5.206 + t^5.237 + t^5.373 + t^5.462 + t^5.551 + 2*t^5.686 + 2*t^5.776 + t^5.865 - 2*t^6. - t^4.422/y - t^4.422*y | detail |