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 |
|---|---|---|---|---|---|---|---|---|---|
| 60092 | SU3adj1nf2 | ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{1}q_{2}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$ | 1.3809 | 1.5734 | 0.8776 | [X:[1.3598], M:[0.7607], q:[0.3064, 0.6265], qb:[0.5335, 0.6128], phi:[0.3201]] | [X:[[12]], M:[[-33]], q:[[13], [7]], qb:[[-10], [26]], phi:[[-6]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{1}$, ${ }q_{1}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{3}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }X_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{1}^{2}$, ${ }\phi_{1}q_{1}^{2}q_{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{1}q_{1}\tilde{q}_{1}$, ${ }M_{1}q_{1}\tilde{q}_{2}$, ${ }M_{1}\phi_{1}^{3}$, ${ }q_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{3}q_{1}^{3}$, ${ }\phi_{1}^{2}q_{1}^{2}q_{2}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }\phi_{1}^{3}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{6}$, ${ }M_{1}q_{2}\tilde{q}_{1}$ | ${}$ | -1 | t^2.28 + t^2.52 + t^2.76 + t^2.88 + 2*t^3.48 + t^3.72 + t^4.08 + 2*t^4.44 + t^4.56 + 3*t^4.68 + t^4.8 + t^5.04 + t^5.16 + t^5.28 + 2*t^5.4 + t^5.52 + 5*t^5.64 + 2*t^5.76 - t^6. + 3*t^6.24 + 3*t^6.36 + t^6.48 + 4*t^6.6 + t^6.72 + t^6.84 + t^6.85 + 3*t^6.96 + t^7.08 + 5*t^7.2 + 3*t^7.32 + 4*t^7.44 + t^7.45 + 5*t^7.56 + 2*t^7.68 + t^7.8 + 5*t^7.92 + 3*t^8.04 + 11*t^8.16 + t^8.27 + 9*t^8.4 + 2*t^8.52 + 3*t^8.64 - 3*t^8.76 + 3*t^8.88 + t^8.88/y^2 - t^3.96/y - t^4.92/y - t^6.24/y - t^6.48/y - t^6.72/y - t^6.84/y - t^7.2/y - (2*t^7.44)/y - t^7.68/y + t^8.04/y + t^8.16/y + t^8.28/y - t^8.4/y - t^8.52/y + t^8.76/y - t^3.96*y - t^4.92*y - t^6.24*y - t^6.48*y - t^6.72*y - t^6.84*y - t^7.2*y - 2*t^7.44*y - t^7.68*y + t^8.04*y + t^8.16*y + t^8.28*y - t^8.4*y - t^8.52*y + t^8.76*y + t^8.88*y^2 | t^2.28/g1^33 + g1^3*t^2.52 + g1^39*t^2.76 + t^2.88/g1^18 + (2*t^3.48)/g1^3 + g1^33*t^3.72 + g1^12*t^4.08 + (2*t^4.44)/g1^9 + t^4.56/g1^66 + 3*g1^27*t^4.68 + t^4.8/g1^30 + g1^6*t^5.04 + t^5.16/g1^51 + g1^42*t^5.28 + (2*t^5.4)/g1^15 + g1^78*t^5.52 + 5*g1^21*t^5.64 + (2*t^5.76)/g1^36 - t^6. + 3*g1^36*t^6.24 + (3*t^6.36)/g1^21 + g1^72*t^6.48 + 4*g1^15*t^6.6 + t^6.72/g1^42 + g1^51*t^6.84 + t^6.85/g1^99 + (3*t^6.96)/g1^6 + t^7.08/g1^63 + 5*g1^30*t^7.2 + (3*t^7.32)/g1^27 + 4*g1^66*t^7.44 + t^7.45/g1^84 + 5*g1^9*t^7.56 + (2*t^7.68)/g1^48 + g1^45*t^7.8 + (5*t^7.92)/g1^12 + (2*t^8.04)/g1^69 + g1^81*t^8.04 + 11*g1^24*t^8.16 + g1^117*t^8.27 + 9*g1^60*t^8.4 + 2*g1^3*t^8.52 + (3*t^8.64)/g1^54 - 3*g1^39*t^8.76 + (3*t^8.88)/g1^18 + t^8.88/(g1^18*y^2) - t^3.96/(g1^6*y) - t^4.92/(g1^12*y) - t^6.24/(g1^39*y) - t^6.48/(g1^3*y) - (g1^33*t^6.72)/y - t^6.84/(g1^24*y) - t^7.2/(g1^45*y) - (2*t^7.44)/(g1^9*y) - (g1^27*t^7.68)/y + (g1^6*t^8.04)/y + t^8.16/(g1^51*y) + (g1^42*t^8.28)/y - t^8.4/(g1^15*y) - t^8.52/(g1^72*y) + t^8.76/(g1^36*y) - (t^3.96*y)/g1^6 - (t^4.92*y)/g1^12 - (t^6.24*y)/g1^39 - (t^6.48*y)/g1^3 - g1^33*t^6.72*y - (t^6.84*y)/g1^24 - (t^7.2*y)/g1^45 - (2*t^7.44*y)/g1^9 - g1^27*t^7.68*y + g1^6*t^8.04*y + (t^8.16*y)/g1^51 + g1^42*t^8.28*y - (t^8.4*y)/g1^15 - (t^8.52*y)/g1^72 + (t^8.76*y)/g1^36 + (t^8.88*y^2)/g1^18 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 57731 | SU3adj1nf2 | ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{1}q_{2}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ | 1.4024 | 1.5963 | 0.8785 | [X:[1.3532], M:[0.7786], q:[0.3662, 0.6896], qb:[0.4721, 0.5317], phi:[0.3234]] | t^2.34 + t^2.51 + t^2.69 + t^2.91 + 2*t^3.49 + t^3.66 + t^4.06 + 2*t^4.46 + 2*t^4.63 + t^4.67 + t^4.85 + t^5.03 + t^5.21 + t^5.24 + t^5.25 + t^5.39 + t^5.4 + 2*t^5.43 + t^5.58 + 2*t^5.6 + 2*t^5.82 - 2*t^6. - t^3.97/y - t^4.94/y - t^3.97*y - t^4.94*y | detail |