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 |
|---|---|---|---|---|---|---|---|---|---|
| 50968 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{3}^{2}$ + ${ }M_{1}M_{2}$ + ${ }M_{2}M_{5}$ + ${ }M_{5}q_{1}\tilde{q}_{2}$ + ${ }M_{6}\phi_{1}^{2}$ | 0.7046 | 0.8662 | 0.8135 | [M:[0.9322, 1.0678, 1.0, 0.8644, 0.9322, 1.0339], q:[0.5, 0.5678], qb:[0.4322, 0.5678], phi:[0.483]] | [M:[[-4], [4], [0], [-8], [-4], [2]], q:[[0], [4]], qb:[[-4], [4]], phi:[[-1]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{4}$, ${ }M_{1}$, ${ }M_{5}$, ${ }M_{3}$, ${ }q_{2}\tilde{q}_{1}$, ${ }M_{6}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{4}^{2}$, ${ }M_{1}M_{4}$, ${ }M_{4}M_{5}$, ${ }M_{1}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{1}M_{5}$, ${ }M_{5}^{2}$, ${ }M_{4}q_{2}\tilde{q}_{1}$, ${ }M_{4}M_{6}$, ${ }M_{1}M_{3}$, ${ }M_{3}M_{5}$, ${ }M_{5}q_{2}\tilde{q}_{1}$, ${ }M_{4}q_{1}\tilde{q}_{2}$, ${ }M_{1}M_{6}$, ${ }M_{5}M_{6}$ | ${}q_{2}^{2}\tilde{q}_{1}^{2}$ | -1 | t^2.593 + 2*t^2.797 + 2*t^3. + t^3.102 + t^3.203 + t^4.042 + t^4.246 + 3*t^4.449 + 2*t^4.653 + 3*t^4.856 + t^5.186 + 2*t^5.39 + 3*t^5.593 + t^5.695 + 2*t^5.797 + 2*t^5.898 - t^6. + 2*t^6.102 - t^6.203 + t^6.305 - t^6.407 + t^6.635 + 3*t^6.839 + 5*t^7.042 + 6*t^7.246 + 6*t^7.449 + 5*t^7.653 + t^7.779 + 3*t^7.856 + 2*t^7.983 + t^8.059 + t^8.085 + 3*t^8.186 + 2*t^8.288 + 2*t^8.39 + 5*t^8.491 - 2*t^8.593 + 6*t^8.695 - 7*t^8.797 + 8*t^8.898 - t^4.449/y - t^7.042/y - t^7.246/y + t^7.653/y + t^7.856/y + (2*t^8.39)/y + (3*t^8.593)/y + t^8.695/y + (5*t^8.797)/y + (2*t^8.898)/y - t^4.449*y - t^7.042*y - t^7.246*y + t^7.653*y + t^7.856*y + 2*t^8.39*y + 3*t^8.593*y + t^8.695*y + 5*t^8.797*y + 2*t^8.898*y | t^2.593/g1^8 + (2*t^2.797)/g1^4 + 2*t^3. + g1^2*t^3.102 + g1^4*t^3.203 + t^4.042/g1^9 + t^4.246/g1^5 + (3*t^4.449)/g1 + 2*g1^3*t^4.653 + 3*g1^7*t^4.856 + t^5.186/g1^16 + (2*t^5.39)/g1^12 + (3*t^5.593)/g1^8 + t^5.695/g1^6 + (2*t^5.797)/g1^4 + (2*t^5.898)/g1^2 - t^6. + 2*g1^2*t^6.102 - g1^4*t^6.203 + g1^6*t^6.305 - g1^8*t^6.407 + t^6.635/g1^17 + (3*t^6.839)/g1^13 + (5*t^7.042)/g1^9 + (6*t^7.246)/g1^5 + (6*t^7.449)/g1 + 5*g1^3*t^7.653 + t^7.779/g1^24 + 3*g1^7*t^7.856 + (2*t^7.983)/g1^20 + g1^11*t^8.059 + t^8.085/g1^18 + (3*t^8.186)/g1^16 + (2*t^8.288)/g1^14 + (2*t^8.39)/g1^12 + (5*t^8.491)/g1^10 - (2*t^8.593)/g1^8 + (6*t^8.695)/g1^6 - (7*t^8.797)/g1^4 + (8*t^8.898)/g1^2 - t^4.449/(g1*y) - t^7.042/(g1^9*y) - t^7.246/(g1^5*y) + (g1^3*t^7.653)/y + (g1^7*t^7.856)/y + (2*t^8.39)/(g1^12*y) + (3*t^8.593)/(g1^8*y) + t^8.695/(g1^6*y) + (5*t^8.797)/(g1^4*y) + (2*t^8.898)/(g1^2*y) - (t^4.449*y)/g1 - (t^7.042*y)/g1^9 - (t^7.246*y)/g1^5 + g1^3*t^7.653*y + g1^7*t^7.856*y + (2*t^8.39*y)/g1^12 + (3*t^8.593*y)/g1^8 + (t^8.695*y)/g1^6 + (5*t^8.797*y)/g1^4 + (2*t^8.898*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 |
|---|---|---|---|---|---|---|---|---|
| 56283 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{3}^{2}$ + ${ }M_{1}M_{2}$ + ${ }M_{2}M_{5}$ + ${ }M_{5}q_{1}\tilde{q}_{2}$ + ${ }M_{6}\phi_{1}^{2}$ + ${ }M_{7}q_{1}\tilde{q}_{2}$ | 0.7115 | 0.8794 | 0.8092 | [M:[0.9178, 1.0822, 1.0, 0.8355, 0.9178, 1.0411, 0.9178], q:[0.5, 0.5822], qb:[0.4178, 0.5822], phi:[0.4794]] | t^2.507 + 3*t^2.753 + 2*t^3. + t^3.123 + t^3.945 + t^4.192 + 3*t^4.438 + 2*t^4.685 + 3*t^4.932 + t^5.013 + 3*t^5.26 + 6*t^5.507 + t^5.63 + 3*t^5.753 + 3*t^5.877 - 3*t^6. - t^4.438/y - t^4.438*y | detail |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 46918 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{3}^{2}$ + ${ }M_{1}M_{2}$ + ${ }M_{2}M_{5}$ + ${ }M_{5}q_{1}\tilde{q}_{2}$ | 0.708 | 0.8725 | 0.8115 | [M:[0.9246, 1.0754, 1.0, 0.8491, 0.9246], q:[0.5, 0.5754], qb:[0.4246, 0.5754], phi:[0.4811]] | t^2.547 + 2*t^2.774 + t^2.887 + 2*t^3. + t^3.226 + t^3.991 + t^4.217 + 3*t^4.443 + 2*t^4.67 + 3*t^4.896 + t^5.095 + 2*t^5.321 + t^5.434 + 3*t^5.547 + 2*t^5.66 + 3*t^5.774 + 2*t^5.887 - t^6. - t^4.443/y - t^4.443*y | detail |