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 |
|---|---|---|---|---|---|---|---|---|---|
| 57595 | SU3adj1nf2 | ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$ + ${ }q_{2}\tilde{q}_{2}X_{1}$ + ${ }M_{1}q_{1}\tilde{q}_{2}$ | 1.2344 | 1.4398 | 0.8573 | [X:[1.4275], M:[0.855], q:[0.7869, 0.2144], qb:[0.4994, 0.3581], phi:[0.3569]] | [X:[[0, 4]], M:[[0, 8]], q:[[-1, -8], [-1, -4]], qb:[[1, 6], [1, 0]], phi:[[0, 1]]] | 2 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}\phi_{1}^{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }M_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{3}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }X_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }\phi_{1}^{3}q_{2}^{3}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}^{5}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{1}$, ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}\phi_{1}^{3}$, ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}q_{2}^{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$ | ${2}\phi_{1}^{4}q_{2}\tilde{q}_{2}$, ${ 2}\phi_{1}^{2}q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$ | 3 | 2*t^2.14 + t^2.57 + t^2.79 + 2*t^3.21 + 2*t^3.86 + 4*t^4.28 + t^4.51 + 2*t^4.71 + 2*t^4.72 + 3*t^4.93 + t^5.13 + 2*t^5.14 + 4*t^5.35 + t^5.58 + 2*t^5.78 + 2*t^5.79 + 3*t^6. + 9*t^6.42 + 2*t^6.43 + 2*t^6.65 + 4*t^6.85 + 4*t^6.86 + 7*t^7.07 + 2*t^7.27 + 4*t^7.28 + t^7.29 + 8*t^7.49 + 2*t^7.51 + t^7.7 + 2*t^7.71 + 4*t^7.72 + 4*t^7.92 + 4*t^7.93 + 6*t^8.14 + 2*t^8.34 + 4*t^8.35 + 2*t^8.36 + 12*t^8.57 + 4*t^8.58 + t^8.79 + 9*t^8.99 - t^4.07/y - t^5.14/y - (2*t^6.21)/y - t^6.64/y - (2*t^7.28)/y + t^7.71/y + t^7.93/y - t^4.07*y - t^5.14*y - 2*t^6.21*y - t^6.64*y - 2*t^7.28*y + t^7.71*y + t^7.93*y | 2*g2^2*t^2.14 + g2^8*t^2.57 + t^2.79/g2^3 + 2*g2^3*t^3.21 + (2*t^3.86)/g2^2 + 4*g2^4*t^4.28 + t^4.51/g2^7 + 2*g2^10*t^4.71 + t^4.72/(g1^3*g2^15) + g1^3*g2^7*t^4.72 + (3*t^4.93)/g2 + g2^16*t^5.13 + t^5.14/(g1^3*g2^9) + g1^3*g2^13*t^5.14 + 4*g2^5*t^5.35 + t^5.58/g2^6 + 2*g2^11*t^5.78 + t^5.79/(g1^3*g2^14) + g1^3*g2^8*t^5.79 + 3*t^6. + 9*g2^6*t^6.42 + t^6.43/(g1^3*g2^19) + g1^3*g2^3*t^6.43 + (2*t^6.65)/g2^5 + 4*g2^12*t^6.85 + (2*t^6.86)/(g1^3*g2^13) + 2*g1^3*g2^9*t^6.86 + 7*g2*t^7.07 + 2*g2^18*t^7.27 + (2*t^7.28)/(g1^3*g2^7) + 2*g1^3*g2^15*t^7.28 + t^7.29/g2^10 + 8*g2^7*t^7.49 + t^7.51/(g1^3*g2^18) + g1^3*g2^4*t^7.51 + g2^24*t^7.7 + t^7.71/(g1^3*g2) + g1^3*g2^21*t^7.71 + (4*t^7.72)/g2^4 + 4*g2^13*t^7.92 + (2*t^7.93)/(g1^3*g2^12) + 2*g1^3*g2^10*t^7.93 + 6*g2^2*t^8.14 + 2*g2^19*t^8.34 + (2*t^8.35)/(g1^3*g2^6) + 2*g1^3*g2^16*t^8.35 + (2*t^8.36)/g2^9 + 12*g2^8*t^8.57 + (2*t^8.58)/(g1^3*g2^17) + 2*g1^3*g2^5*t^8.58 + t^8.79/g2^3 + 9*g2^14*t^8.99 - (g2*t^4.07)/y - (g2^2*t^5.14)/y - (2*g2^3*t^6.21)/y - (g2^9*t^6.64)/y - (2*g2^4*t^7.28)/y + (g2^10*t^7.71)/y + t^7.93/(g2*y) - g2*t^4.07*y - g2^2*t^5.14*y - 2*g2^3*t^6.21*y - g2^9*t^6.64*y - 2*g2^4*t^7.28*y + g2^10*t^7.71*y + (t^7.93*y)/g2 |
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 |
|---|---|---|---|---|---|---|---|---|
| 58596 | ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$ + ${ }q_{2}\tilde{q}_{2}X_{1}$ + ${ }M_{1}q_{1}\tilde{q}_{2}$ + ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$ | 1.1867 | 1.3914 | 0.8529 | [X:[1.4518], M:[0.9036], q:[0.6692, 0.121], qb:[0.6049, 0.4272], phi:[0.3629]] | 2*t^2.18 + t^2.71 + t^2.73 + 2*t^3.27 + 3*t^3.82 + 5*t^4.36 + t^4.38 + 2*t^4.89 + 4*t^4.91 + t^5.42 + 4*t^5.44 + 3*t^5.47 + 2*t^5.98 + 6*t^6. - t^4.09/y - t^5.18/y - t^4.09*y - t^5.18*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 |
|---|---|---|---|---|---|---|---|---|---|
| 47925 | SU3adj1nf2 | ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$ + ${ }q_{2}\tilde{q}_{2}X_{1}$ | 1.2241 | 1.4234 | 0.86 | [X:[1.459], q:[0.7527, 0.2117], qb:[0.5178, 0.3292], phi:[0.3648]] | 2*t^2.189 + t^2.717 + t^3.246 + 2*t^3.283 + 2*t^3.811 + t^4.34 + 4*t^4.377 + 2*t^4.623 + 3*t^4.906 + 2*t^5.189 + 3*t^5.434 + 3*t^5.471 + 2*t^5.717 + t^5.963 + 3*t^6. - t^4.094/y - t^5.189/y - t^4.094*y - t^5.189*y | detail |