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 |
|---|---|---|---|---|---|---|---|---|---|
| 58601 | SU3adj1nf2 | ${}M_{1}\phi_{1}^{3}$ + ${ }M_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{2}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ | 1.3966 | 1.5747 | 0.8869 | [X:[1.3833], M:[1.075, 0.775], q:[0.5288, 0.5205], qb:[0.3962, 0.7045], phi:[0.3083]] | [X:[[0, 2]], M:[[0, 3], [0, -9]], q:[[-1, -4], [-1, 9]], qb:[[1, 1], [1, 0]], phi:[[0, -1]]] | 2 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{1}$, ${ }M_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }X_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{2}^{2}$, ${ }M_{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }q_{1}q_{2}\tilde{q}_{1}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }M_{1}M_{2}$, ${ }q_{1}^{2}\tilde{q}_{1}^{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }\phi_{1}q_{1}^{2}q_{2}$ | ${}$ | -3 | t^2.33 + t^2.75 + t^2.78 + t^3.22 + t^3.67 + 2*t^3.7 + t^4.15 + 2*t^4.6 + 2*t^4.63 + t^4.65 + t^5.1 + t^5.42 + t^5.5 + 2*t^5.52 + 3*t^5.55 + t^5.63 + t^5.66 - 3*t^6. + t^6.03 + 3*t^6.34 + t^6.42 + 4*t^6.45 + 3*t^6.48 + t^6.56 + t^6.58 + t^6.9 + t^6.95 + t^6.98 - t^7.03 + 2*t^7.27 + 3*t^7.35 + 7*t^7.37 + 5*t^7.4 + t^7.43 + t^7.46 + t^7.48 + t^7.51 + t^7.53 - 2*t^7.72 - t^7.74 + t^7.82 + t^7.85 + 2*t^7.88 - t^7.93 - 2*t^7.96 + t^8.17 + 2*t^8.19 + t^8.25 + 4*t^8.27 + 9*t^8.3 + 4*t^8.33 + t^8.35 + t^8.38 + 2*t^8.41 + t^8.43 - 2*t^8.64 - 4*t^8.75 - 2*t^8.78 + 2*t^8.8 - t^8.86 - 2*t^8.88 - t^8.91 + t^8.78/y^2 - t^3.93/y - t^4.85/y - t^6.25/y - t^6.67/y - t^6.7/y - t^7.15/y - t^7.18/y - t^7.6/y - (2*t^7.63)/y + t^8.1/y - t^8.55/y - t^8.58/y + t^8.97/y - t^3.93*y - t^4.85*y - t^6.25*y - t^6.67*y - t^6.7*y - t^7.15*y - t^7.18*y - t^7.6*y - 2*t^7.63*y + t^8.1*y - t^8.55*y - t^8.58*y + t^8.97*y + t^8.78*y^2 | t^2.33/g2^9 + g2^10*t^2.75 + t^2.78/g2^3 + g2^3*t^3.22 + g2^9*t^3.67 + (2*t^3.7)/g2^4 + g2^2*t^4.15 + 2*g2^8*t^4.6 + (2*t^4.63)/g2^5 + t^4.65/g2^18 + t^5.1/g2^12 + g1^3*g2*t^5.42 + g2^20*t^5.5 + 2*g2^7*t^5.52 + (3*t^5.55)/g2^6 + (g2^13*t^5.63)/g1^3 + t^5.66/g1^3 - 3*t^6. + t^6.03/g2^13 + 3*g1^3*t^6.34 + g2^19*t^6.42 + 4*g2^6*t^6.45 + (3*t^6.48)/g2^7 + (g2^12*t^6.56)/g1^3 + t^6.58/(g1^3*g2) + g2^12*t^6.9 + t^6.95/g2^14 + t^6.98/g2^27 - (g2^5*t^7.03)/g1^3 + (2*g1^3*t^7.27)/g2 + 3*g2^18*t^7.35 + 7*g2^5*t^7.37 + (5*t^7.4)/g2^8 + t^7.43/g2^21 + (g2^24*t^7.46)/g1^3 + (g2^11*t^7.48)/g1^3 + t^7.51/(g1^3*g2^2) + t^7.53/(g1^3*g2^15) - 2*g1^3*g2^5*t^7.72 - (g1^3*t^7.74)/g2^8 + g2^11*t^7.82 + t^7.85/g2^2 + (2*t^7.88)/g2^15 - (g2^17*t^7.93)/g1^3 - (2*g2^4*t^7.96)/g1^3 + g1^3*g2^11*t^8.17 + (2*g1^3*t^8.19)/g2^2 + g2^30*t^8.25 + 4*g2^17*t^8.27 + 9*g2^4*t^8.3 + (4*t^8.33)/g2^9 + t^8.35/g2^22 + (g2^23*t^8.38)/g1^3 + (2*g2^10*t^8.41)/g1^3 + t^8.43/(g1^3*g2^3) - 2*g1^3*g2^4*t^8.64 - 4*g2^10*t^8.75 - (2*t^8.78)/g2^3 + (2*t^8.8)/g2^16 - (g2^16*t^8.86)/g1^3 - (2*g2^3*t^8.88)/g1^3 - t^8.91/(g1^3*g2^10) + t^8.78/(g2^3*y^2) - t^3.93/(g2*y) - t^4.85/(g2^2*y) - t^6.25/(g2^10*y) - (g2^9*t^6.67)/y - t^6.7/(g2^4*y) - (g2^2*t^7.15)/y - t^7.18/(g2^11*y) - (g2^8*t^7.6)/y - (2*t^7.63)/(g2^5*y) + t^8.1/(g2^12*y) - t^8.55/(g2^6*y) - t^8.58/(g2^19*y) + (g2^13*t^8.97)/y - (t^3.93*y)/g2 - (t^4.85*y)/g2^2 - (t^6.25*y)/g2^10 - g2^9*t^6.67*y - (t^6.7*y)/g2^4 - g2^2*t^7.15*y - (t^7.18*y)/g2^11 - g2^8*t^7.6*y - (2*t^7.63*y)/g2^5 + (t^8.1*y)/g2^12 - (t^8.55*y)/g2^6 - (t^8.58*y)/g2^19 + g2^13*t^8.97*y + (t^8.78*y^2)/g2^3 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 57651 | SU3adj1nf2 | ${}M_{1}\phi_{1}^{3}$ + ${ }M_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{2}\phi_{1}q_{2}\tilde{q}_{1}$ | 1.4955 | 1.727 | 0.8659 | [X:[], M:[0.99, 0.6722], q:[0.5044, 0.4856], qb:[0.5056, 0.4844], phi:[0.3367]] | 2*t^2.02 + t^2.91 + 3*t^2.97 + t^3.03 + t^3.92 + t^3.98 + t^4.03 + 3*t^4.04 + 3*t^4.93 + t^4.98 + 7*t^4.99 + 3*t^5.05 + t^5.43 + t^5.44 + t^5.49 + t^5.5 + t^5.82 + 3*t^5.88 + t^5.93 + 5*t^5.94 + t^5.95 + t^5.99 - t^4.01/y - t^5.02/y - t^4.01*y - t^5.02*y | detail |