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 |
|---|---|---|---|---|---|---|---|---|---|
| 56768 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{1}\tilde{q}_{2}$ + ${ }M_{5}\phi_{1}^{2}$ + ${ }M_{2}M_{3}$ + ${ }M_{1}^{2}$ + ${ }M_{2}M_{6}$ + ${ }M_{5}M_{7}$ | 0.7049 | 0.8679 | 0.8122 | [M:[1.0, 1.0619, 0.9381, 0.8763, 1.0309, 0.9381, 0.9691], q:[0.4227, 0.5773], qb:[0.5155, 0.5464], phi:[0.4845]] | [M:[[0], [4], [-4], [-8], [2], [-4], [-2]], q:[[-5], [5]], qb:[[1], [3]], phi:[[-1]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{4}$, ${ }M_{3}$, ${ }M_{6}$, ${ }M_{7}$, ${ }\phi_{1}^{2}$, ${ }M_{1}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{4}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{4}M_{6}$, ${ }M_{4}M_{7}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{3}^{2}$, ${ }M_{1}M_{4}$, ${ }M_{3}M_{6}$, ${ }M_{6}^{2}$, ${ }M_{3}M_{7}$, ${ }M_{6}M_{7}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{1}M_{3}$, ${ }M_{1}M_{6}$, ${ }M_{7}^{2}$, ${ }M_{7}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }M_{1}M_{7}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{4}q_{2}\tilde{q}_{1}$ | ${}$ | -3 | t^2.629 + 2*t^2.814 + 2*t^2.907 + t^3. + t^3.278 + t^3.99 + t^4.268 + t^4.361 + t^4.454 + t^4.546 + t^4.639 + 2*t^4.732 + t^4.825 + t^4.918 + t^5.258 + 2*t^5.443 + t^5.536 + 3*t^5.629 + 3*t^5.722 + 4*t^5.814 + t^5.907 - 3*t^6. - t^6.371 - t^6.464 + t^6.557 + t^6.618 + 2*t^6.804 + 3*t^6.897 + t^6.99 + t^7.082 + 3*t^7.175 + 5*t^7.268 + 3*t^7.361 + t^7.454 + 4*t^7.546 + 3*t^7.639 + 3*t^7.732 + t^7.886 - t^7.918 + t^7.979 + 2*t^8.072 + t^8.165 + t^8.196 + 4*t^8.258 + 2*t^8.35 + 5*t^8.443 + 4*t^8.536 + 3*t^8.629 + 6*t^8.722 - 5*t^8.814 - 5*t^8.907 - t^4.454/y - t^7.082/y - t^7.268/y - t^7.361/y + t^7.546/y + t^7.639/y + t^7.825/y + (2*t^8.443)/y + (2*t^8.536)/y + (2*t^8.629)/y + (4*t^8.722)/y + (3*t^8.814)/y + (3*t^8.907)/y - t^4.454*y - t^7.082*y - t^7.268*y - t^7.361*y + t^7.546*y + t^7.639*y + t^7.825*y + 2*t^8.443*y + 2*t^8.536*y + 2*t^8.629*y + 4*t^8.722*y + 3*t^8.814*y + 3*t^8.907*y | t^2.629/g1^8 + (2*t^2.814)/g1^4 + (2*t^2.907)/g1^2 + t^3. + g1^6*t^3.278 + t^3.99/g1^11 + t^4.268/g1^5 + t^4.361/g1^3 + t^4.454/g1 + g1*t^4.546 + g1^3*t^4.639 + 2*g1^5*t^4.732 + g1^7*t^4.825 + g1^9*t^4.918 + t^5.258/g1^16 + (2*t^5.443)/g1^12 + t^5.536/g1^10 + (3*t^5.629)/g1^8 + (3*t^5.722)/g1^6 + (4*t^5.814)/g1^4 + t^5.907/g1^2 - 3*t^6. - g1^8*t^6.371 - g1^10*t^6.464 + g1^12*t^6.557 + t^6.618/g1^19 + (2*t^6.804)/g1^15 + (3*t^6.897)/g1^13 + t^6.99/g1^11 + t^7.082/g1^9 + (3*t^7.175)/g1^7 + (5*t^7.268)/g1^5 + (3*t^7.361)/g1^3 + t^7.454/g1 + 4*g1*t^7.546 + 3*g1^3*t^7.639 + 3*g1^5*t^7.732 + t^7.886/g1^24 - g1^9*t^7.918 + t^7.979/g1^22 + (2*t^8.072)/g1^20 + t^8.165/g1^18 + g1^15*t^8.196 + (4*t^8.258)/g1^16 + (2*t^8.35)/g1^14 + (5*t^8.443)/g1^12 + (4*t^8.536)/g1^10 + (3*t^8.629)/g1^8 + (6*t^8.722)/g1^6 - (5*t^8.814)/g1^4 - (5*t^8.907)/g1^2 - t^4.454/(g1*y) - t^7.082/(g1^9*y) - t^7.268/(g1^5*y) - t^7.361/(g1^3*y) + (g1*t^7.546)/y + (g1^3*t^7.639)/y + (g1^7*t^7.825)/y + (2*t^8.443)/(g1^12*y) + (2*t^8.536)/(g1^10*y) + (2*t^8.629)/(g1^8*y) + (4*t^8.722)/(g1^6*y) + (3*t^8.814)/(g1^4*y) + (3*t^8.907)/(g1^2*y) - (t^4.454*y)/g1 - (t^7.082*y)/g1^9 - (t^7.268*y)/g1^5 - (t^7.361*y)/g1^3 + g1*t^7.546*y + g1^3*t^7.639*y + g1^7*t^7.825*y + (2*t^8.443*y)/g1^12 + (2*t^8.536*y)/g1^10 + (2*t^8.629*y)/g1^8 + (4*t^8.722*y)/g1^6 + (3*t^8.814*y)/g1^4 + (3*t^8.907*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 |
|---|---|---|---|---|---|---|---|---|---|
| 55058 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{1}\tilde{q}_{2}$ + ${ }M_{5}\phi_{1}^{2}$ + ${ }M_{2}M_{3}$ + ${ }M_{1}^{2}$ + ${ }M_{2}M_{6}$ | 0.7022 | 0.8628 | 0.8139 | [M:[1.0, 1.0555, 0.9445, 0.889, 1.0277, 0.9445], q:[0.4306, 0.5694], qb:[0.5139, 0.5416], phi:[0.4861]] | t^2.667 + 2*t^2.834 + t^2.917 + t^3. + t^3.083 + t^3.25 + t^4.042 + t^4.292 + t^4.375 + t^4.458 + t^4.542 + t^4.625 + 2*t^4.708 + t^4.791 + t^4.875 + t^5.334 + 2*t^5.501 + 3*t^5.667 + 2*t^5.75 + 2*t^5.834 + 2*t^5.917 - 2*t^6. - t^4.458/y - t^4.458*y | detail |