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 |
|---|---|---|---|---|---|---|---|---|---|
| 46454 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}X_{1}$ + ${ }M_{3}\phi_{1}q_{1}^{2}$ + ${ }M_{4}q_{1}\tilde{q}_{1}$ + ${ }M_{5}q_{2}\tilde{q}_{2}$ | 0.6312 | 0.7837 | 0.8054 | [X:[1.6], M:[1.2, 0.4, 0.7599, 0.7866, 0.8134], q:[0.42, 0.38], qb:[0.7933, 0.8067], phi:[0.4]] | [X:[[0, 0]], M:[[0, 0], [0, 0], [2, 0], [1, 1], [-1, -1]], q:[[-1, 0], [1, 0]], qb:[[0, -1], [0, 1]], phi:[[0, 0]]] | 2 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{3}$, ${ }M_{4}$, ${ }\phi_{1}^{2}$, ${ }M_{5}$, ${ }\phi_{1}q_{2}^{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }M_{1}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{3}M_{5}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{4}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{4}M_{5}$, ${ }\phi_{1}^{4}$, ${ }X_{1}$, ${ }M_{5}\phi_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{5}^{2}$, ${ }M_{3}\phi_{1}q_{2}^{2}$, ${ }M_{3}q_{2}\tilde{q}_{1}$, ${ }M_{4}\phi_{1}q_{2}^{2}$, ${ }M_{1}M_{3}$, ${ }M_{3}\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}^{3}q_{2}^{2}$, ${ }M_{4}q_{2}\tilde{q}_{1}$, ${ }M_{5}\phi_{1}q_{2}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }M_{5}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{1}M_{4}$, ${ }M_{4}\phi_{1}q_{1}q_{2}$, ${ }M_{3}q_{1}\tilde{q}_{2}$ | ${}\phi_{1}^{3}q_{1}q_{2}$ | -1 | t^2.28 + t^2.36 + t^2.4 + t^2.44 + t^3.48 + t^3.52 + 2*t^3.6 + t^3.68 + t^4.559 + t^4.64 + t^4.68 + 2*t^4.72 + t^4.76 + 3*t^4.8 + t^4.84 + t^4.88 + t^5.759 + t^5.8 + t^5.84 + 3*t^5.88 + t^5.92 + 3*t^5.96 - t^6. + 2*t^6.04 + t^6.839 + t^6.919 + 2*t^6.959 + 3*t^7. + 2*t^7.04 + 4*t^7.08 + 2*t^7.12 + 3*t^7.16 + 2*t^7.2 + t^7.24 + t^7.28 - t^7.32 + t^7.36 + t^8.039 + t^8.079 + t^8.119 + 3*t^8.159 + 2*t^8.2 + 4*t^8.24 + 4*t^8.32 - 2*t^8.36 + 2*t^8.4 - 3*t^8.44 + t^8.48 - 2*t^8.52 - t^4.2/y - t^6.48/y - t^6.56/y - t^6.64/y + t^7.64/y + t^7.68/y + t^7.72/y + (2*t^7.76)/y + t^7.8/y + (2*t^7.84)/y + t^7.92/y + t^8.8/y + (4*t^8.88)/y + (4*t^8.96)/y - t^4.2*y - t^6.48*y - t^6.56*y - t^6.64*y + t^7.64*y + t^7.68*y + t^7.72*y + 2*t^7.76*y + t^7.8*y + 2*t^7.84*y + t^7.92*y + t^8.8*y + 4*t^8.88*y + 4*t^8.96*y | g1^2*t^2.28 + g1*g2*t^2.36 + t^2.4 + t^2.44/(g1*g2) + g1^2*t^3.48 + (g1*t^3.52)/g2 + 2*t^3.6 + (g2*t^3.68)/g1 + g1^4*t^4.559 + g1^3*g2*t^4.64 + g1^2*t^4.68 + (g1*t^4.72)/g2 + g1^2*g2^2*t^4.72 + g1*g2*t^4.76 + 3*t^4.8 + t^4.84/(g1*g2) + t^4.88/(g1^2*g2^2) + g1^4*t^5.759 + (g1^3*t^5.8)/g2 + g1^3*g2*t^5.84 + 3*g1^2*t^5.88 + (g1*t^5.92)/g2 + t^5.96/g2^2 + 2*g1*g2*t^5.96 - t^6. + t^6.04/(g1*g2) + g2^2*t^6.04 + g1^6*t^6.839 + g1^5*g2*t^6.919 + 2*g1^4*t^6.959 + (2*g1^3*t^7.)/g2 + g1^4*g2^2*t^7. + (g1^2*t^7.04)/g2^2 + g1^3*g2*t^7.04 + 3*g1^2*t^7.08 + g1^3*g2^3*t^7.08 + (g1*t^7.12)/g2 + g1^2*g2^2*t^7.12 + t^7.16/g2^2 + 2*g1*g2*t^7.16 + 2*t^7.2 + t^7.24/(g1*g2) + t^7.28/(g1^2*g2^2) - (2*t^7.32)/g1^2 + t^7.32/(g1^3*g2^3) + (g2^2*t^7.36)/g1^2 + g1^6*t^8.039 + (g1^5*t^8.079)/g2 + g1^5*g2*t^8.119 + 3*g1^4*t^8.159 + (g1^3*t^8.2)/g2 + g1^4*g2^2*t^8.2 + (g1^2*t^8.24)/g2^2 + 3*g1^3*g2*t^8.24 + (2*g1*t^8.32)/g2 + 2*g1^2*g2^2*t^8.32 + t^8.36/g2^2 - 3*g1*g2*t^8.36 + t^8.4/(g1*g2^3) + g1*g2^3*t^8.4 - (3*t^8.44)/(g1*g2) + t^8.48/(g1^2*g2^2) - (2*t^8.52)/g1^2 - t^4.2/y - (g1^2*t^6.48)/y - (g1*g2*t^6.56)/y - t^6.64/(g1*g2*y) + (g1^3*g2*t^7.64)/y + (g1^2*t^7.68)/y + (g1*t^7.72)/(g2*y) + (2*g1*g2*t^7.76)/y + t^7.8/y + (2*t^7.84)/(g1*g2*y) + t^7.92/(g1^2*y) + (g1^3*t^8.8)/(g2*y) + (4*g1^2*t^8.88)/y + (g1*t^8.92)/(g2*y) - (g1^2*g2^2*t^8.92)/y + t^8.96/(g2^2*y) + (3*g1*g2*t^8.96)/y - t^4.2*y - g1^2*t^6.48*y - g1*g2*t^6.56*y - (t^6.64*y)/(g1*g2) + g1^3*g2*t^7.64*y + g1^2*t^7.68*y + (g1*t^7.72*y)/g2 + 2*g1*g2*t^7.76*y + t^7.8*y + (2*t^7.84*y)/(g1*g2) + (t^7.92*y)/g1^2 + (g1^3*t^8.8*y)/g2 + 4*g1^2*t^8.88*y + (g1*t^8.92*y)/g2 - g1^2*g2^2*t^8.92*y + (t^8.96*y)/g2^2 + 3*g1*g2*t^8.96*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 |
|---|---|---|---|---|---|---|---|---|
| 48155 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}X_{1}$ + ${ }M_{3}\phi_{1}q_{1}^{2}$ + ${ }M_{4}q_{1}\tilde{q}_{1}$ + ${ }M_{5}q_{2}\tilde{q}_{2}$ + ${ }M_{5}\phi_{1}q_{2}^{2}$ | 0.6308 | 0.7823 | 0.8063 | [X:[1.6], M:[1.2, 0.4, 0.7748, 0.7748, 0.8252], q:[0.4126, 0.3874], qb:[0.8126, 0.7874], phi:[0.4]] | 2*t^2.324 + t^2.4 + t^2.476 + t^3.524 + 4*t^3.6 + 3*t^4.649 + 2*t^4.724 + 4*t^4.8 + t^4.876 + t^4.951 + 2*t^5.849 + 7*t^5.924 - t^4.2/y - t^4.2*y | detail | |
| 47073 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}X_{1}$ + ${ }M_{3}\phi_{1}q_{1}^{2}$ + ${ }M_{4}q_{1}\tilde{q}_{1}$ + ${ }M_{5}q_{2}\tilde{q}_{2}$ + ${ }M_{6}q_{2}\tilde{q}_{1}$ | 0.6475 | 0.812 | 0.7974 | [X:[1.6], M:[1.2, 0.4, 0.7839, 0.7678, 0.8322, 0.7839], q:[0.4081, 0.3919], qb:[0.8242, 0.7758], phi:[0.4]] | t^2.303 + 2*t^2.352 + t^2.4 + t^2.497 + 2*t^3.552 + 2*t^3.6 + t^4.607 + 2*t^4.655 + 4*t^4.703 + 2*t^4.752 + 3*t^4.8 + 2*t^4.848 + t^4.897 + t^4.993 + 2*t^5.855 + 5*t^5.903 + 4*t^5.952 - t^6. - t^4.2/y - t^4.2*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 |
|---|---|---|---|---|---|---|---|---|---|
| 46196 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}X_{1}$ + ${ }M_{3}\phi_{1}q_{1}^{2}$ + ${ }M_{4}q_{1}\tilde{q}_{1}$ | 0.6169 | 0.7615 | 0.8102 | [X:[1.6], M:[1.2, 0.4, 0.7434, 0.7434], q:[0.4283, 0.3717], qb:[0.8283, 0.7717], phi:[0.4]] | 2*t^2.23 + t^2.4 + 2*t^3.43 + 4*t^3.6 + 3*t^4.46 + 2*t^4.63 + 2*t^4.8 + 4*t^5.66 + 8*t^5.83 - t^6. - t^4.2/y - t^4.2*y | detail |