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 |
|---|---|---|---|---|---|---|---|---|---|
| 1127 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{4}q_{1}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{5}\phi_{1}q_{2}^{2}$ + ${ }M_{1}M_{6}$ | 0.6892 | 0.8559 | 0.8053 | [M:[1.0233, 1.1111, 0.9767, 0.7545, 0.7133, 0.9767], q:[0.7778, 0.4211], qb:[0.5556, 0.4678], phi:[0.4444]] | [M:[[1], [0], [-1], [-1], [2], [-1]], q:[[0], [-1]], qb:[[0], [1]], phi:[[0]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{5}$, ${ }M_{4}$, ${ }\phi_{1}^{2}$, ${ }M_{3}$, ${ }M_{6}$, ${ }M_{2}$, ${ }q_{1}q_{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{5}^{2}$, ${ }M_{4}M_{5}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{4}^{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{3}M_{5}$, ${ }M_{5}M_{6}$, ${ }M_{3}M_{4}$, ${ }M_{4}M_{6}$, ${ }\phi_{1}^{4}$, ${ }M_{2}M_{5}$, ${ }M_{2}M_{4}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{3}^{2}$, ${ }M_{3}M_{6}$, ${ }M_{6}^{2}$, ${ }M_{4}q_{1}q_{2}$ | ${}$ | -2 | t^2.14 + t^2.263 + t^2.667 + 2*t^2.93 + t^3.333 + t^3.597 + 2*t^4. + t^4.14 + t^4.263 + t^4.28 + 2*t^4.403 + t^4.527 + t^4.667 + t^4.807 + t^4.93 + 2*t^5.07 + 2*t^5.193 + t^5.333 + t^5.473 + 2*t^5.597 + 3*t^5.86 - 2*t^6. + t^6.14 + 3*t^6.263 + t^6.28 + t^6.42 + 3*t^6.527 + 2*t^6.543 + 2*t^6.667 + t^6.79 + 2*t^6.807 + 4*t^6.93 + t^6.946 + t^7.07 + 2*t^7.193 + 2*t^7.21 + 3*t^7.333 + 2*t^7.457 + 3*t^7.597 + t^7.613 + t^7.737 + 2*t^7.86 + 4*t^8. + 3*t^8.124 - t^8.14 - t^8.263 + 2*t^8.28 + t^8.403 + t^8.42 + 3*t^8.527 + t^8.543 + t^8.559 + 2*t^8.683 + 5*t^8.79 + 2*t^8.807 - 2*t^8.93 + 2*t^8.946 - t^4.333/y - t^6.473/y - t^6.597/y - t^7.263/y + (2*t^7.403)/y + t^7.807/y + t^7.93/y + (3*t^8.07)/y + (3*t^8.193)/y + t^8.473/y + (3*t^8.597)/y - t^8.613/y + t^8.86/y - t^4.333*y - t^6.473*y - t^6.597*y - t^7.263*y + 2*t^7.403*y + t^7.807*y + t^7.93*y + 3*t^8.07*y + 3*t^8.193*y + t^8.473*y + 3*t^8.597*y - t^8.613*y + t^8.86*y | g1^2*t^2.14 + t^2.263/g1 + t^2.667 + (2*t^2.93)/g1 + t^3.333 + t^3.597/g1 + 2*t^4. + g1^2*t^4.14 + t^4.263/g1 + g1^4*t^4.28 + 2*g1*t^4.403 + t^4.527/g1^2 + t^4.667 + g1^2*t^4.807 + t^4.93/g1 + 2*g1*t^5.07 + (2*t^5.193)/g1^2 + t^5.333 + g1^2*t^5.473 + (2*t^5.597)/g1 + (3*t^5.86)/g1^2 - 2*t^6. + g1^2*t^6.14 + (3*t^6.263)/g1 + g1^4*t^6.28 + g1^6*t^6.42 + (3*t^6.527)/g1^2 + 2*g1^3*t^6.543 + 2*t^6.667 + t^6.79/g1^3 + 2*g1^2*t^6.807 + (4*t^6.93)/g1 + g1^4*t^6.946 + g1*t^7.07 + (2*t^7.193)/g1^2 + 2*g1^3*t^7.21 + 3*t^7.333 + (2*t^7.457)/g1^3 + (3*t^7.597)/g1 + g1^4*t^7.613 + g1*t^7.737 + (2*t^7.86)/g1^2 + 4*t^8. + (3*t^8.124)/g1^3 - g1^2*t^8.14 - t^8.263/g1 + 2*g1^4*t^8.28 + g1*t^8.403 + g1^6*t^8.42 + (3*t^8.527)/g1^2 + g1^3*t^8.543 + g1^8*t^8.559 + 2*g1^5*t^8.683 + (5*t^8.79)/g1^3 + 2*g1^2*t^8.807 - (2*t^8.93)/g1 + 2*g1^4*t^8.946 - t^4.333/y - (g1^2*t^6.473)/y - t^6.597/(g1*y) - t^7.263/(g1*y) + (2*g1*t^7.403)/y + (g1^2*t^7.807)/y + t^7.93/(g1*y) + (3*g1*t^8.07)/y + (3*t^8.193)/(g1^2*y) + (g1^2*t^8.473)/y + (3*t^8.597)/(g1*y) - (g1^4*t^8.613)/y + t^8.86/(g1^2*y) - t^4.333*y - g1^2*t^6.473*y - (t^6.597*y)/g1 - (t^7.263*y)/g1 + 2*g1*t^7.403*y + g1^2*t^7.807*y + (t^7.93*y)/g1 + 3*g1*t^8.07*y + (3*t^8.193*y)/g1^2 + g1^2*t^8.473*y + (3*t^8.597*y)/g1 - g1^4*t^8.613*y + (t^8.86*y)/g1^2 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 697 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{4}q_{1}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{5}\phi_{1}q_{2}^{2}$ | 0.6877 | 0.8539 | 0.8054 | [M:[1.0082, 1.1111, 0.9918, 0.7695, 0.6831], q:[0.7778, 0.4362], qb:[0.5556, 0.4527], phi:[0.4444]] | t^2.049 + t^2.309 + t^2.667 + t^2.975 + t^3.025 + t^3.333 + t^3.642 + 2*t^4. + t^4.049 + t^4.099 + t^4.309 + 2*t^4.358 + t^4.617 + t^4.667 + t^4.716 + t^4.975 + t^5.025 + t^5.074 + t^5.284 + 2*t^5.333 + t^5.383 + t^5.642 + t^5.691 + t^5.951 - t^6. - t^4.333/y - t^4.333*y | detail |