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 |
|---|---|---|---|---|---|---|---|---|---|
| 57147 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{3}M_{4}$ + ${ }M_{5}\phi_{1}^{2}$ + ${ }M_{6}\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{7}q_{1}\tilde{q}_{2}$ | 0.6688 | 0.8425 | 0.7938 | [M:[1.06, 0.6999, 0.8199, 1.1801, 1.06, 0.6999, 1.0498], q:[0.5351, 0.4049], qb:[0.765, 0.4151], phi:[0.47]] | [M:[[4], [-20], [-12], [12], [4], [-20], [-30]], q:[[19], [-23]], qb:[[1], [11]], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{2}$, ${ }M_{6}$, ${ }M_{3}$, ${ }M_{7}$, ${ }M_{1}$, ${ }M_{5}$, ${ }q_{2}\tilde{q}_{1}$, ${ }M_{4}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{2}^{2}$, ${ }M_{2}M_{6}$, ${ }M_{6}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{2}M_{3}$, ${ }M_{3}M_{6}$, ${ }\phi_{1}q_{1}^{2}$, ${ }M_{3}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{2}M_{7}$, ${ }M_{6}M_{7}$, ${ }M_{1}M_{2}$, ${ }M_{2}M_{5}$, ${ }M_{1}M_{6}$, ${ }M_{5}M_{6}$, ${ }M_{3}M_{7}$, ${ }M_{2}q_{2}\tilde{q}_{1}$, ${ }M_{6}q_{2}\tilde{q}_{1}$, ${ }M_{1}M_{3}$, ${ }M_{2}M_{4}$, ${ }M_{3}M_{5}$, ${ }M_{4}M_{6}$, ${ }M_{2}\phi_{1}q_{2}^{2}$, ${ }M_{6}\phi_{1}q_{2}^{2}$, ${ }M_{2}\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{6}\phi_{1}q_{2}\tilde{q}_{2}$ | ${}$ | -2 | 2*t^2.1 + t^2.46 + t^3.149 + 2*t^3.18 + t^3.51 + t^3.54 + t^3.839 + t^3.87 + 3*t^4.199 + t^4.23 + t^4.261 + 2*t^4.559 + t^4.621 + t^4.92 + 2*t^5.249 + 4*t^5.28 + 2*t^5.609 + 3*t^5.64 + 2*t^5.939 + 2*t^5.969 - 2*t^6. - t^6.031 + 6*t^6.299 + 4*t^6.329 + 2*t^6.36 - t^6.391 + 4*t^6.659 + 2*t^6.69 + 3*t^6.72 + t^6.988 + 4*t^7.019 - t^7.08 + 4*t^7.349 + 8*t^7.379 + t^7.678 + 4*t^7.709 + 5*t^7.739 + 3*t^8.038 + 4*t^8.069 - 3*t^8.1 - 3*t^8.13 + 9*t^8.398 + 7*t^8.429 + 2*t^8.46 - 3*t^8.49 + 7*t^8.759 + 4*t^8.789 + 3*t^8.82 + t^8.881 - t^4.41/y - (2*t^6.51)/y + t^7.199/y + t^7.23/y + t^7.261/y + t^7.559/y - t^7.59/y + (2*t^8.249)/y + (4*t^8.28)/y + (2*t^8.31)/y + (4*t^8.64)/y + (2*t^8.939)/y + (3*t^8.969)/y - t^4.41*y - 2*t^6.51*y + t^7.199*y + t^7.23*y + t^7.261*y + t^7.559*y - t^7.59*y + 2*t^8.249*y + 4*t^8.28*y + 2*t^8.31*y + 4*t^8.64*y + 2*t^8.939*y + 3*t^8.969*y | (2*t^2.1)/g1^20 + t^2.46/g1^12 + t^3.149/g1^30 + 2*g1^4*t^3.18 + t^3.51/g1^22 + g1^12*t^3.54 + t^3.839/g1^48 + t^3.87/g1^14 + (3*t^4.199)/g1^40 + t^4.23/g1^6 + g1^28*t^4.261 + (2*t^4.559)/g1^32 + g1^36*t^4.621 + t^4.92/g1^24 + (2*t^5.249)/g1^50 + (4*t^5.28)/g1^16 + (2*t^5.609)/g1^42 + (3*t^5.64)/g1^8 + (2*t^5.939)/g1^68 + (2*t^5.969)/g1^34 - 2*t^6. - g1^34*t^6.031 + (6*t^6.299)/g1^60 + (4*t^6.329)/g1^26 + 2*g1^8*t^6.36 - g1^42*t^6.391 + (4*t^6.659)/g1^52 + (2*t^6.69)/g1^18 + 3*g1^16*t^6.72 + t^6.988/g1^78 + (4*t^7.019)/g1^44 - g1^24*t^7.08 + (4*t^7.349)/g1^70 + (8*t^7.379)/g1^36 + t^7.678/g1^96 + (4*t^7.709)/g1^62 + (5*t^7.739)/g1^28 + (3*t^8.038)/g1^88 + (4*t^8.069)/g1^54 - (3*t^8.1)/g1^20 - 3*g1^14*t^8.13 + (9*t^8.398)/g1^80 + (7*t^8.429)/g1^46 + (2*t^8.46)/g1^12 - 3*g1^22*t^8.49 + (7*t^8.759)/g1^72 + (4*t^8.789)/g1^38 + (3*t^8.82)/g1^4 + g1^64*t^8.881 - t^4.41/(g1^2*y) - (2*t^6.51)/(g1^22*y) + t^7.199/(g1^40*y) + t^7.23/(g1^6*y) + (g1^28*t^7.261)/y + t^7.559/(g1^32*y) - (g1^2*t^7.59)/y + (2*t^8.249)/(g1^50*y) + (4*t^8.28)/(g1^16*y) + (2*g1^18*t^8.31)/y + (4*t^8.64)/(g1^8*y) + (2*t^8.939)/(g1^68*y) + (3*t^8.969)/(g1^34*y) - (t^4.41*y)/g1^2 - (2*t^6.51*y)/g1^22 + (t^7.199*y)/g1^40 + (t^7.23*y)/g1^6 + g1^28*t^7.261*y + (t^7.559*y)/g1^32 - g1^2*t^7.59*y + (2*t^8.249*y)/g1^50 + (4*t^8.28*y)/g1^16 + 2*g1^18*t^8.31*y + (4*t^8.64*y)/g1^8 + (2*t^8.939*y)/g1^68 + (3*t^8.969*y)/g1^34 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 55570 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{3}M_{4}$ + ${ }M_{5}\phi_{1}^{2}$ + ${ }M_{6}\phi_{1}\tilde{q}_{2}^{2}$ | 0.6751 | 0.8503 | 0.7939 | [M:[1.0552, 0.7242, 0.8345, 1.1655, 1.0552, 0.7242], q:[0.512, 0.4329], qb:[0.7638, 0.4017], phi:[0.4724]] | 2*t^2.173 + t^2.504 + t^2.741 + 2*t^3.165 + t^3.496 + t^3.59 + t^3.921 + t^4.015 + t^4.158 + t^4.252 + 3*t^4.345 + t^4.489 + 2*t^4.676 + 2*t^4.914 + t^5.007 + t^5.245 + 4*t^5.338 + t^5.482 + 3*t^5.669 + t^5.763 + t^5.906 - 2*t^6. - t^4.417/y - t^4.417*y | detail |