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 |
|---|---|---|---|---|---|---|---|---|---|
| 1666 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{4}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{1}\tilde{q}_{2}$ + ${ }M_{2}M_{4}$ + ${ }M_{6}\phi_{1}q_{2}^{2}$ + ${ }M_{7}\phi_{1}\tilde{q}_{2}^{2}$ | 0.6797 | 0.8677 | 0.7834 | [M:[0.8077, 1.2, 0.7923, 0.8, 0.7923, 0.8154, 0.7846], q:[0.8, 0.3923], qb:[0.8, 0.4077], phi:[0.4]] | [M:[[1], [0], [-1], [0], [-1], [2], [-2]], q:[[0], [-1]], qb:[[0], [1]], phi:[[0]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{7}$, ${ }M_{3}$, ${ }M_{5}$, ${ }M_{4}$, ${ }\phi_{1}^{2}$, ${ }M_{1}$, ${ }M_{6}$, ${ }q_{1}q_{2}$, ${ }M_{2}$, ${ }M_{7}^{2}$, ${ }M_{3}M_{7}$, ${ }M_{5}M_{7}$, ${ }M_{3}^{2}$, ${ }M_{3}M_{5}$, ${ }M_{5}^{2}$, ${ }M_{4}M_{7}$, ${ }M_{7}\phi_{1}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{4}M_{5}$, ${ }M_{1}M_{7}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{1}M_{3}$, ${ }M_{4}^{2}$, ${ }M_{1}M_{5}$, ${ }M_{6}M_{7}$, ${ }M_{4}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }q_{1}\tilde{q}_{1}$, ${ }M_{1}M_{4}$, ${ }M_{3}M_{6}$, ${ }M_{5}M_{6}$, ${ }M_{1}\phi_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }M_{4}M_{6}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{1}M_{6}$, ${ }M_{6}^{2}$, ${ }M_{7}q_{1}q_{2}$, ${ }M_{2}M_{7}$, ${ }M_{3}q_{1}q_{2}$, ${ }M_{5}q_{1}q_{2}$, ${ }M_{2}M_{3}$, ${ }M_{2}M_{5}$, ${ }M_{4}q_{1}q_{2}$ | ${}\phi_{1}\tilde{q}_{1}^{2}$ | 0 | t^2.354 + 2*t^2.377 + 2*t^2.4 + t^2.423 + t^2.446 + t^3.577 + t^3.6 + t^4.707 + 2*t^4.73 + 5*t^4.754 + 5*t^4.777 + 7*t^4.8 + 4*t^4.823 + 3*t^4.846 + t^4.87 + t^4.893 + t^5.93 + 2*t^5.954 + 2*t^5.977 + t^7.061 + 2*t^7.084 + 5*t^7.107 + 9*t^7.13 + 12*t^7.154 + 12*t^7.177 + 12*t^7.2 + 7*t^7.223 + 7*t^7.246 + 5*t^7.27 + 3*t^7.293 + t^7.316 + t^7.339 + t^8.284 + 2*t^8.307 + 3*t^8.33 - 3*t^8.377 - 4*t^8.4 - 6*t^8.423 - 4*t^8.446 - t^8.47 - t^4.2/y - t^6.554/y - (2*t^6.577)/y - t^6.6/y - t^6.623/y - t^6.646/y + (2*t^7.73)/y + (4*t^7.754)/y + (6*t^7.777)/y + (5*t^7.8)/y + (6*t^7.823)/y + (3*t^7.846)/y + t^7.87/y - t^8.907/y - t^8.93/y - t^8.954/y + t^8.977/y - t^4.2*y - t^6.554*y - 2*t^6.577*y - t^6.6*y - t^6.623*y - t^6.646*y + 2*t^7.73*y + 4*t^7.754*y + 6*t^7.777*y + 5*t^7.8*y + 6*t^7.823*y + 3*t^7.846*y + t^7.87*y - t^8.907*y - t^8.93*y - t^8.954*y + t^8.977*y | t^2.354/g1^2 + (2*t^2.377)/g1 + 2*t^2.4 + g1*t^2.423 + g1^2*t^2.446 + t^3.577/g1 + t^3.6 + t^4.707/g1^4 + (2*t^4.73)/g1^3 + (5*t^4.754)/g1^2 + (5*t^4.777)/g1 + 7*t^4.8 + 4*g1*t^4.823 + 3*g1^2*t^4.846 + g1^3*t^4.87 + g1^4*t^4.893 + t^5.93/g1^3 + (2*t^5.954)/g1^2 + (2*t^5.977)/g1 + t^7.061/g1^6 + (2*t^7.084)/g1^5 + (5*t^7.107)/g1^4 + (9*t^7.13)/g1^3 + (12*t^7.154)/g1^2 + (12*t^7.177)/g1 + 12*t^7.2 + 7*g1*t^7.223 + 7*g1^2*t^7.246 + 5*g1^3*t^7.27 + 3*g1^4*t^7.293 + g1^5*t^7.316 + g1^6*t^7.339 + t^8.284/g1^5 + (2*t^8.307)/g1^4 + (3*t^8.33)/g1^3 - (3*t^8.377)/g1 - 4*t^8.4 - 6*g1*t^8.423 - 4*g1^2*t^8.446 - g1^3*t^8.47 - t^4.2/y - t^6.554/(g1^2*y) - (2*t^6.577)/(g1*y) - t^6.6/y - (g1*t^6.623)/y - (g1^2*t^6.646)/y + (2*t^7.73)/(g1^3*y) + (4*t^7.754)/(g1^2*y) + (6*t^7.777)/(g1*y) + (5*t^7.8)/y + (6*g1*t^7.823)/y + (3*g1^2*t^7.846)/y + (g1^3*t^7.87)/y - t^8.907/(g1^4*y) - t^8.93/(g1^3*y) - t^8.954/(g1^2*y) + t^8.977/(g1*y) - t^4.2*y - (t^6.554*y)/g1^2 - (2*t^6.577*y)/g1 - t^6.6*y - g1*t^6.623*y - g1^2*t^6.646*y + (2*t^7.73*y)/g1^3 + (4*t^7.754*y)/g1^2 + (6*t^7.777*y)/g1 + 5*t^7.8*y + 6*g1*t^7.823*y + 3*g1^2*t^7.846*y + g1^3*t^7.87*y - (t^8.907*y)/g1^4 - (t^8.93*y)/g1^3 - (t^8.954*y)/g1^2 + (t^8.977*y)/g1 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 1070 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{4}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{1}\tilde{q}_{2}$ + ${ }M_{2}M_{4}$ + ${ }M_{6}\phi_{1}q_{2}^{2}$ | 0.6633 | 0.8389 | 0.7907 | [M:[0.7907, 1.2, 0.8093, 0.8, 0.8093, 0.7814], q:[0.8, 0.4093], qb:[0.8, 0.3907], phi:[0.4]] | t^2.344 + t^2.372 + 2*t^2.4 + 2*t^2.428 + t^3.544 + t^3.6 + t^3.628 + t^4.689 + t^4.717 + 3*t^4.744 + 4*t^4.772 + 6*t^4.8 + 4*t^4.828 + 3*t^4.856 + t^5.889 + t^5.917 + 2*t^5.944 + 2*t^5.972 - t^4.2/y - t^4.2*y | detail |