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 |
|---|---|---|---|---|---|---|---|---|---|
| 46873 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }\phi_{1}^{4}$ + ${ }M_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{1}\tilde{q}_{2}$ + ${ }M_{3}\phi_{1}q_{2}^{2}$ + ${ }M_{4}q_{2}\tilde{q}_{1}$ + ${ }M_{5}q_{1}\tilde{q}_{1}$ | 0.6385 | 0.8121 | 0.7862 | [X:[], M:[1.1113, 0.75, 0.7226, 1.25, 0.8887], q:[0.75, 0.3887], qb:[0.3613, 0.5], phi:[0.5]] | [X:[], M:[[1], [0], [2], [0], [-1]], q:[[0], [-1]], qb:[[1], [0]], phi:[[0]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{3}$, ${ }M_{2}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{5}$, ${ }\phi_{1}^{2}$, ${ }M_{1}$, ${ }q_{1}q_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{4}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }M_{2}M_{3}$, ${ }M_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}M_{5}$, ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}M_{5}$, ${ }M_{3}\phi_{1}^{2}$, ${ }\tilde{q}_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{5}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{5}^{2}$, ${ }M_{1}M_{3}$, ${ }M_{1}M_{2}$, ${ }M_{3}q_{1}q_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{2}q_{1}q_{2}$, ${ }M_{3}\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{2}\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{3}q_{1}\tilde{q}_{2}$ | ${}M_{2}M_{4}$, ${ }M_{1}M_{5}$ | 1 | t^2.17 + t^2.25 + t^2.58 + t^2.67 + t^3. + t^3.33 + t^3.42 + t^3.67 + 2*t^3.75 + t^4.08 + t^4.17 + t^4.34 + t^4.42 + 2*t^4.5 + t^4.75 + 2*t^4.83 + t^4.92 + 2*t^5.17 + 2*t^5.25 + t^5.33 + t^5.5 + 2*t^5.58 + t^5.67 + t^5.84 + 3*t^5.92 + t^6. + 2*t^6.25 + 3*t^6.33 + t^6.42 + t^6.5 + t^6.59 + 4*t^6.67 + 3*t^6.75 + t^6.83 + t^6.92 + 3*t^7. + 3*t^7.08 + t^7.17 + 3*t^7.34 + 4*t^7.42 + 3*t^7.5 + t^7.67 + 4*t^7.75 + 3*t^7.83 + t^7.92 + 2*t^8. + 3*t^8.09 + 3*t^8.17 + t^8.25 + 2*t^8.42 + 4*t^8.5 + t^8.58 + t^8.75 + 5*t^8.84 + 4*t^8.92 - t^4.5/y - t^6.67/y + t^7.42/y + t^7.75/y + (2*t^7.83)/y + t^7.92/y + t^8.17/y + (2*t^8.25)/y + t^8.33/y + t^8.5/y + (3*t^8.58)/y + (2*t^8.67)/y + (4*t^8.92)/y - t^4.5*y - t^6.67*y + t^7.42*y + t^7.75*y + 2*t^7.83*y + t^7.92*y + t^8.17*y + 2*t^8.25*y + t^8.33*y + t^8.5*y + 3*t^8.58*y + 2*t^8.67*y + 4*t^8.92*y | g1^2*t^2.17 + t^2.25 + g1*t^2.58 + t^2.67/g1 + t^3. + g1*t^3.33 + t^3.42/g1 + g1^2*t^3.67 + 2*t^3.75 + g1*t^4.08 + t^4.17/g1 + g1^4*t^4.34 + g1^2*t^4.42 + 2*t^4.5 + g1^3*t^4.75 + 2*g1*t^4.83 + t^4.92/g1 + 2*g1^2*t^5.17 + 2*t^5.25 + t^5.33/g1^2 + g1^3*t^5.5 + 2*g1*t^5.58 + t^5.67/g1 + g1^4*t^5.84 + 3*g1^2*t^5.92 + t^6. + 2*g1^3*t^6.25 + 3*g1*t^6.33 + t^6.42/g1 + g1^6*t^6.5 + g1^4*t^6.59 + 4*g1^2*t^6.67 + 3*t^6.75 + t^6.83/g1^2 + g1^5*t^6.92 + 3*g1^3*t^7. + 3*g1*t^7.08 + t^7.17/g1 + 3*g1^4*t^7.34 + 4*g1^2*t^7.42 + 3*t^7.5 + g1^5*t^7.67 + 4*g1^3*t^7.75 + 3*g1*t^7.83 + t^7.92/g1 + t^8./g1^3 + g1^6*t^8. + 3*g1^4*t^8.09 + 3*g1^2*t^8.17 + t^8.25 + 2*g1^5*t^8.42 + 4*g1^3*t^8.5 + g1*t^8.58 - t^8.67/g1 + g1^8*t^8.67 + g1^6*t^8.75 + 5*g1^4*t^8.84 + 4*g1^2*t^8.92 - t^4.5/y - (g1^2*t^6.67)/y + (g1^2*t^7.42)/y + (g1^3*t^7.75)/y + (2*g1*t^7.83)/y + t^7.92/(g1*y) + (g1^2*t^8.17)/y + (2*t^8.25)/y + t^8.33/(g1^2*y) + (g1^3*t^8.5)/y + (3*g1*t^8.58)/y + (2*t^8.67)/(g1*y) + (4*g1^2*t^8.92)/y - t^4.5*y - g1^2*t^6.67*y + g1^2*t^7.42*y + g1^3*t^7.75*y + 2*g1*t^7.83*y + (t^7.92*y)/g1 + g1^2*t^8.17*y + 2*t^8.25*y + (t^8.33*y)/g1^2 + g1^3*t^8.5*y + 3*g1*t^8.58*y + (2*t^8.67*y)/g1 + 4*g1^2*t^8.92*y |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 46712 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }\phi_{1}^{4}$ + ${ }M_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{1}\tilde{q}_{2}$ + ${ }M_{3}\phi_{1}q_{2}^{2}$ + ${ }M_{4}q_{2}\tilde{q}_{1}$ | 0.629 | 0.7983 | 0.788 | [X:[], M:[1.0975, 0.75, 0.6949, 1.25], q:[0.75, 0.4025], qb:[0.3475, 0.5], phi:[0.5]] | t^2.08 + t^2.25 + t^2.54 + t^3. + 2*t^3.29 + t^3.46 + t^3.58 + 2*t^3.75 + t^4.04 + t^4.17 + t^4.21 + t^4.33 + 2*t^4.5 + t^4.63 + t^4.79 + 2*t^5.08 + t^5.25 + 2*t^5.38 + 3*t^5.54 + t^5.67 + 4*t^5.83 - t^4.5/y - t^4.5*y | detail |