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 |
|---|---|---|---|---|---|---|---|---|---|
| 5016 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{5}^{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{1}M_{6}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}X_{1}$ + ${ }M_{7}\phi_{1}q_{2}^{2}$ + ${ }M_{8}\phi_{1}q_{1}q_{2}$ | 0.632 | 0.8013 | 0.7888 | [X:[1.6], M:[1.2, 0.4, 0.9081, 0.6919, 1.0, 0.8, 0.8919, 0.8], q:[0.446, 0.354], qb:[0.646, 0.954], phi:[0.4]] | [X:[[0]], M:[[0], [0], [2], [-2], [0], [0], [-2], [0]], q:[[-1], [1]], qb:[[-1], [1]], phi:[[0]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{4}$, ${ }M_{6}$, ${ }M_{8}$, ${ }\phi_{1}^{2}$, ${ }M_{7}$, ${ }M_{3}$, ${ }M_{5}$, ${ }\phi_{1}q_{1}^{2}$, ${ }M_{4}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{4}M_{6}$, ${ }M_{4}M_{8}$, ${ }M_{4}\phi_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{4}M_{7}$, ${ }M_{3}M_{4}$, ${ }M_{6}^{2}$, ${ }M_{6}M_{8}$, ${ }M_{8}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{8}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }X_{1}$, ${ }M_{4}M_{5}$, ${ }M_{6}M_{7}$, ${ }M_{7}M_{8}$, ${ }M_{7}\phi_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{3}M_{6}$, ${ }M_{3}M_{8}$, ${ }M_{3}\phi_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{7}^{2}$, ${ }M_{5}M_{6}$, ${ }M_{3}M_{7}$, ${ }M_{5}M_{8}$, ${ }M_{5}\phi_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }M_{4}\phi_{1}q_{1}^{2}$ | ${}$ | -2 | t^2.076 + 3*t^2.4 + t^2.676 + t^2.724 + t^3. + t^3.876 + t^4.151 + t^4.2 + 3*t^4.476 + t^4.751 + 8*t^4.8 + 4*t^5.076 + 3*t^5.124 + t^5.351 + 3*t^5.4 + t^5.449 + t^5.951 - 2*t^6. + t^6.227 + 3*t^6.276 - t^6.324 + 4*t^6.551 + t^6.6 + t^6.827 + 8*t^6.876 - t^6.924 + 4*t^7.151 + 12*t^7.2 + t^7.427 + 8*t^7.476 + 6*t^7.524 + 4*t^7.751 + 4*t^7.8 + 3*t^7.849 + 2*t^8.027 - 2*t^8.076 - t^8.124 + t^8.173 + t^8.303 + 3*t^8.351 - 9*t^8.4 + 4*t^8.627 + t^8.676 - 7*t^8.724 + t^8.903 + 10*t^8.951 - t^4.2/y - t^6.276/y - (2*t^6.6)/y - t^6.876/y - t^6.924/y + (4*t^7.476)/y + t^7.524/y + t^7.751/y + (6*t^7.8)/y + (4*t^8.076)/y + (4*t^8.124)/y - t^8.351/y + (4*t^8.4)/y - t^8.676/y + t^8.724/y - t^4.2*y - t^6.276*y - 2*t^6.6*y - t^6.876*y - t^6.924*y + 4*t^7.476*y + t^7.524*y + t^7.751*y + 6*t^7.8*y + 4*t^8.076*y + 4*t^8.124*y - t^8.351*y + 4*t^8.4*y - t^8.676*y + t^8.724*y | t^2.076/g1^2 + 3*t^2.4 + t^2.676/g1^2 + g1^2*t^2.724 + t^3. + t^3.876/g1^2 + t^4.151/g1^4 + t^4.2 + (3*t^4.476)/g1^2 + t^4.751/g1^4 + 8*t^4.8 + (4*t^5.076)/g1^2 + 3*g1^2*t^5.124 + t^5.351/g1^4 + 3*t^5.4 + g1^4*t^5.449 + t^5.951/g1^4 - 2*t^6. + t^6.227/g1^6 + (3*t^6.276)/g1^2 - g1^2*t^6.324 + (4*t^6.551)/g1^4 + t^6.6 + t^6.827/g1^6 + (8*t^6.876)/g1^2 - g1^2*t^6.924 + (4*t^7.151)/g1^4 + 12*t^7.2 + t^7.427/g1^6 + (8*t^7.476)/g1^2 + 6*g1^2*t^7.524 + (4*t^7.751)/g1^4 + 4*t^7.8 + 3*g1^4*t^7.849 + (2*t^8.027)/g1^6 - (2*t^8.076)/g1^2 - g1^2*t^8.124 + g1^6*t^8.173 + t^8.303/g1^8 + (3*t^8.351)/g1^4 - 9*t^8.4 + (4*t^8.627)/g1^6 + t^8.676/g1^2 - 7*g1^2*t^8.724 + t^8.903/g1^8 + (10*t^8.951)/g1^4 - t^4.2/y - t^6.276/(g1^2*y) - (2*t^6.6)/y - t^6.876/(g1^2*y) - (g1^2*t^6.924)/y + (4*t^7.476)/(g1^2*y) + (g1^2*t^7.524)/y + t^7.751/(g1^4*y) + (6*t^7.8)/y + (4*t^8.076)/(g1^2*y) + (4*g1^2*t^8.124)/y - t^8.351/(g1^4*y) + (4*t^8.4)/y - t^8.676/(g1^2*y) + (g1^2*t^8.724)/y - t^4.2*y - (t^6.276*y)/g1^2 - 2*t^6.6*y - (t^6.876*y)/g1^2 - g1^2*t^6.924*y + (4*t^7.476*y)/g1^2 + g1^2*t^7.524*y + (t^7.751*y)/g1^4 + 6*t^7.8*y + (4*t^8.076*y)/g1^2 + 4*g1^2*t^8.124*y - (t^8.351*y)/g1^4 + 4*t^8.4*y - (t^8.676*y)/g1^2 + g1^2*t^8.724*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 |
|---|---|---|---|---|---|---|---|---|---|
| 3149 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{5}^{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{1}M_{6}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}X_{1}$ + ${ }M_{7}\phi_{1}q_{2}^{2}$ | 0.6155 | 0.7723 | 0.797 | [X:[1.6], M:[1.2, 0.4, 0.9081, 0.6919, 1.0, 0.8, 0.8919], q:[0.446, 0.354], qb:[0.646, 0.954], phi:[0.4]] | t^2.076 + 2*t^2.4 + t^2.676 + t^2.724 + t^3. + t^3.6 + t^3.876 + t^4.151 + t^4.2 + 2*t^4.476 + t^4.751 + 5*t^4.8 + 3*t^5.076 + 2*t^5.124 + t^5.351 + 2*t^5.4 + t^5.449 + t^5.676 + t^5.951 - t^4.2/y - t^4.2*y | detail |