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 |
|---|---|---|---|---|---|---|---|---|---|
| 3225 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{3}\phi_{1}q_{2}^{2}$ + ${ }M_{3}M_{4}$ | 0.5839 | 0.7416 | 0.7873 | [M:[0.9509, 1.1472, 0.8528, 1.1472], q:[0.7377, 0.3114], qb:[0.4095, 0.4432], phi:[0.5245]] | [M:[[4], [-12], [12], [-12]], q:[[1], [-5]], qb:[[-13], [25]], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}q_{2}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }M_{1}$, ${ }\phi_{1}^{2}$, ${ }M_{2}$, ${ }M_{4}$, ${ }\phi_{1}q_{2}^{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }M_{4}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}^{3}\tilde{q}_{1}$, ${ }M_{1}^{2}$, ${ }M_{4}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{3}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$ | ${}\phi_{1}q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$ | -1 | t^2.163 + t^2.264 + t^2.853 + t^3.147 + 3*t^3.442 + t^3.543 + t^3.736 + t^3.837 + t^4.031 + t^4.132 + t^4.233 + t^4.325 + t^4.426 + t^4.528 + t^5.015 + t^5.117 + t^5.31 + t^5.411 + 2*t^5.604 + 3*t^5.706 + t^5.807 - t^6. + t^6.193 + 2*t^6.294 + t^6.396 + t^6.488 + t^6.497 + 3*t^6.589 + t^6.69 + t^6.791 + 5*t^6.883 + 2*t^6.985 + t^7.086 + 3*t^7.178 + 2*t^7.279 + 2*t^7.38 + 3*t^7.472 + t^7.574 + 3*t^7.675 + 3*t^7.767 + t^7.776 + t^7.868 + 2*t^7.969 + t^8.061 + 2*t^8.07 - t^8.163 - t^8.264 + t^8.356 + t^8.365 + t^8.457 + t^8.466 + t^8.558 + t^8.65 + t^8.659 + t^8.752 + t^8.761 - t^8.853 - t^4.574/y + t^7.132/y + t^7.426/y + t^8.117/y + t^8.31/y + t^8.411/y + (3*t^8.604)/y + (4*t^8.706)/y + t^8.807/y + t^8.899/y - t^4.574*y + t^7.132*y + t^7.426*y + t^8.117*y + t^8.31*y + t^8.411*y + 3*t^8.604*y + 4*t^8.706*y + t^8.807*y + t^8.899*y | t^2.163/g1^18 + g1^20*t^2.264 + g1^4*t^2.853 + t^3.147/g1^4 + (3*t^3.442)/g1^12 + g1^26*t^3.543 + t^3.736/g1^20 + g1^18*t^3.837 + t^4.031/g1^28 + g1^10*t^4.132 + g1^48*t^4.233 + t^4.325/g1^36 + g1^2*t^4.426 + g1^40*t^4.528 + t^5.015/g1^14 + g1^24*t^5.117 + t^5.31/g1^22 + g1^16*t^5.411 + (2*t^5.604)/g1^30 + 3*g1^8*t^5.706 + g1^46*t^5.807 - t^6. + t^6.193/g1^46 + (2*t^6.294)/g1^8 + g1^30*t^6.396 + t^6.488/g1^54 + g1^68*t^6.497 + (3*t^6.589)/g1^16 + g1^22*t^6.69 + g1^60*t^6.791 + (5*t^6.883)/g1^24 + 2*g1^14*t^6.985 + g1^52*t^7.086 + (3*t^7.178)/g1^32 + 2*g1^6*t^7.279 + 2*g1^44*t^7.38 + (3*t^7.472)/g1^40 + t^7.574/g1^2 + 3*g1^36*t^7.675 + (3*t^7.767)/g1^48 + g1^74*t^7.776 + t^7.868/g1^10 + 2*g1^28*t^7.969 + t^8.061/g1^56 + 2*g1^66*t^8.07 - t^8.163/g1^18 - g1^20*t^8.264 + t^8.356/g1^64 + g1^58*t^8.365 + t^8.457/g1^26 + g1^96*t^8.466 + g1^12*t^8.558 + t^8.65/g1^72 + g1^50*t^8.659 + t^8.752/g1^34 + g1^88*t^8.761 - g1^4*t^8.853 - t^4.574/(g1^2*y) + (g1^10*t^7.132)/y + (g1^2*t^7.426)/y + (g1^24*t^8.117)/y + t^8.31/(g1^22*y) + (g1^16*t^8.411)/y + (3*t^8.604)/(g1^30*y) + (4*g1^8*t^8.706)/y + (g1^46*t^8.807)/y + t^8.899/(g1^38*y) - (t^4.574*y)/g1^2 + g1^10*t^7.132*y + g1^2*t^7.426*y + g1^24*t^8.117*y + (t^8.31*y)/g1^22 + g1^16*t^8.411*y + (3*t^8.604*y)/g1^30 + 4*g1^8*t^8.706*y + g1^46*t^8.807*y + (t^8.899*y)/g1^38 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 2715 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{3}\phi_{1}q_{2}^{2}$ | 0.597 | 0.7645 | 0.7809 | [M:[0.9486, 1.1541, 0.8459], q:[0.7372, 0.3142], qb:[0.4169, 0.429], phi:[0.5257]] | t^2.193 + t^2.23 + t^2.538 + t^2.846 + t^3.154 + 2*t^3.462 + t^3.499 + t^3.77 + t^3.807 + t^4.078 + t^4.115 + t^4.151 + t^4.387 + t^4.423 + t^4.459 + t^4.731 + t^4.767 + t^5.039 + 2*t^5.076 + t^5.347 + 2*t^5.384 + t^5.655 + 3*t^5.692 + t^5.728 + t^6. - t^4.577/y - t^4.577*y | detail |