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 |
|---|---|---|---|---|---|---|---|---|---|
| 3778 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}^{2}$ + ${ }M_{2}M_{3}$ + ${ }\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{4}X_{1}$ + ${ }M_{5}\phi_{1}q_{1}^{2}$ + ${ }M_{6}\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{7}\phi_{1}^{2}$ | 0.5778 | 0.7207 | 0.8018 | [X:[1.5714], M:[1.0, 0.7143, 1.2857, 0.4286, 0.9107, 0.8036, 1.1429], q:[0.3304, 0.6696], qb:[0.3839, 0.9018], phi:[0.4286]] | [X:[[0]], M:[[0], [0], [0], [0], [-2], [2], [0]], q:[[1], [-1]], qb:[[-1], [1]], phi:[[0]]] | 1 | {a: 50739/87808, c: 63283/87808, X1: 11/7, M1: 1, M2: 5/7, M3: 9/7, M4: 3/7, M5: 51/56, M6: 45/56, M7: 8/7, q1: 37/112, q2: 75/112, qb1: 43/112, qb2: 101/112, phi1: 3/7} |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{2}$, ${ }M_{6}$, ${ }M_{5}$, ${ }M_{1}$, ${ }q_{2}\tilde{q}_{1}$, ${ }M_{7}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{3}$, ${ }M_{2}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{2}M_{6}$, ${ }X_{1}$, ${ }M_{6}^{2}$, ${ }M_{2}M_{5}$, ${ }M_{1}M_{2}$, ${ }M_{5}M_{6}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{1}M_{6}$, ${ }M_{5}^{2}$, ${ }M_{2}M_{7}$, ${ }M_{6}q_{2}\tilde{q}_{1}$, ${ }M_{6}M_{7}$, ${ }M_{6}\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{5}q_{2}\tilde{q}_{1}$ | ${}$ | -1 | t^2.143 + t^2.411 + t^2.732 + t^3. + t^3.161 + 2*t^3.429 + t^3.696 + t^3.857 + t^4.286 + t^4.554 + t^4.714 + t^4.821 + t^4.875 + 2*t^5.143 + t^5.304 + t^5.411 + t^5.464 + 2*t^5.571 + 2*t^5.839 + t^5.893 - t^6. + t^6.107 + 2*t^6.161 + t^6.321 + 2*t^6.429 + 2*t^6.589 + t^6.696 + 2*t^6.857 + t^6.964 + t^7.125 + t^7.232 + t^7.286 + t^7.393 + t^7.446 + 2*t^7.554 + t^7.607 + 2*t^7.714 + t^7.821 + t^7.875 + t^7.982 + t^8.036 - t^8.143 + t^8.196 + 2*t^8.25 + t^8.304 - 2*t^8.411 + t^8.464 + t^8.518 + 3*t^8.571 + t^8.625 - t^8.732 + t^8.839 + t^8.893 - t^4.286/y - t^6.696/y - t^7.018/y + (2*t^7.554)/y + (2*t^7.875)/y + (2*t^8.143)/y + t^8.304/y + t^8.411/y + (3*t^8.571)/y + t^8.732/y + (3*t^8.839)/y + t^8.893/y - t^4.286*y - t^6.696*y - t^7.018*y + 2*t^7.554*y + 2*t^7.875*y + 2*t^8.143*y + t^8.304*y + t^8.411*y + 3*t^8.571*y + t^8.732*y + 3*t^8.839*y + t^8.893*y | t^2.143 + g1^2*t^2.411 + t^2.732/g1^2 + t^3. + t^3.161/g1^2 + 2*t^3.429 + g1^2*t^3.696 + t^3.857 + t^4.286 + g1^2*t^4.554 + t^4.714 + g1^4*t^4.821 + t^4.875/g1^2 + 2*t^5.143 + t^5.304/g1^2 + g1^2*t^5.411 + t^5.464/g1^4 + 2*t^5.571 + 2*g1^2*t^5.839 + t^5.893/g1^4 - t^6. + g1^4*t^6.107 + (2*t^6.161)/g1^2 + t^6.321/g1^4 + 2*t^6.429 + (2*t^6.589)/g1^2 + g1^2*t^6.696 + 2*t^6.857 + g1^4*t^6.964 + g1^2*t^7.125 + g1^6*t^7.232 + t^7.286 + g1^4*t^7.393 + t^7.446/g1^2 + 2*g1^2*t^7.554 + t^7.607/g1^4 + 2*t^7.714 + g1^4*t^7.821 + t^7.875/g1^2 + g1^2*t^7.982 + t^8.036/g1^4 - t^8.143 + t^8.196/g1^6 + 2*g1^4*t^8.25 + t^8.304/g1^2 - 2*g1^2*t^8.411 + t^8.464/g1^4 + g1^6*t^8.518 + 3*t^8.571 + t^8.625/g1^6 - t^8.732/g1^2 + g1^2*t^8.839 + t^8.893/g1^4 - t^4.286/y - (g1^2*t^6.696)/y - t^7.018/(g1^2*y) + (2*g1^2*t^7.554)/y + (2*t^7.875)/(g1^2*y) + (2*t^8.143)/y + t^8.304/(g1^2*y) + (g1^2*t^8.411)/y + (3*t^8.571)/y + t^8.732/(g1^2*y) + (3*g1^2*t^8.839)/y + t^8.893/(g1^4*y) - t^4.286*y - g1^2*t^6.696*y - (t^7.018*y)/g1^2 + 2*g1^2*t^7.554*y + (2*t^7.875*y)/g1^2 + 2*t^8.143*y + (t^8.304*y)/g1^2 + g1^2*t^8.411*y + 3*t^8.571*y + (t^8.732*y)/g1^2 + 3*g1^2*t^8.839*y + (t^8.893*y)/g1^4 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 3334 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}^{2}$ + ${ }M_{2}M_{3}$ + ${ }\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{4}X_{1}$ + ${ }M_{5}\phi_{1}q_{1}^{2}$ + ${ }M_{6}\phi_{1}\tilde{q}_{1}^{2}$ | 0.5904 | 0.7422 | 0.7955 | [X:[1.5714], M:[1.0, 0.7143, 1.2857, 0.4286, 0.9107, 0.8036], q:[0.3304, 0.6696], qb:[0.3839, 0.9018], phi:[0.4286]] | t^2.143 + t^2.411 + t^2.571 + t^2.732 + t^3. + t^3.161 + t^3.429 + t^3.696 + t^3.857 + t^4.286 + t^4.554 + 2*t^4.714 + t^4.821 + t^4.875 + t^4.982 + 3*t^5.143 + 2*t^5.304 + t^5.411 + t^5.464 + 2*t^5.571 + t^5.732 + t^5.839 + t^5.893 - t^4.286/y - t^4.286*y | detail | {a: 51843/87808, c: 65171/87808, X1: 11/7, M1: 1, M2: 5/7, M3: 9/7, M4: 3/7, M5: 51/56, M6: 45/56, q1: 37/112, q2: 75/112, qb1: 43/112, qb2: 101/112, phi1: 3/7} |