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 |
|---|---|---|---|---|---|---|---|---|---|
| 60781 | SU3adj1nf2 | ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }\phi_{1}q_{1}^{2}q_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{1}q_{1}\tilde{q}_{1}$ | 1.3977 | 1.5928 | 0.8775 | [X:[1.3407], M:[0.8352], q:[0.6667, 0.337], qb:[0.4982, 0.5203], phi:[0.3296]] | [X:[[4]], M:[[1]], q:[[0], [2]], qb:[[-1], [11]], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{1}$, ${ }q_{2}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{3}$, ${ }q_{1}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }X_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }M_{1}q_{2}\tilde{q}_{1}$, ${ }M_{1}q_{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}\phi_{1}^{3}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$ | ${}\phi_{1}^{2}q_{1}q_{2}^{2}$, ${ }\phi_{1}^{3}q_{2}^{3}$ | 0 | 2*t^2.51 + t^2.57 + t^2.97 + t^3.49 + 2*t^3.56 + t^4.02 + 2*t^4.48 + 2*t^4.55 + 3*t^5.01 + 2*t^5.08 + t^5.14 + 3*t^5.47 + 3*t^5.54 + t^5.61 + 4*t^6.07 + 2*t^6.13 + t^6.46 + 5*t^6.53 + 2*t^6.59 - t^6.92 + 3*t^6.99 + 6*t^7.06 + 5*t^7.12 + t^7.45 + 5*t^7.52 + 5*t^7.58 + 3*t^7.65 + t^7.72 - t^7.91 + 4*t^7.98 + 9*t^8.04 + 8*t^8.11 + t^8.18 - t^8.44 - t^8.51 + 5*t^8.57 + 4*t^8.64 + 2*t^8.7 + 3*t^8.97 + t^8.97/y^2 - t^3.99/y - t^4.98/y - (2*t^6.49)/y - t^6.56/y - t^6.96/y - (2*t^7.48)/y - (2*t^7.55)/y - t^7.94/y + t^8.01/y + (2*t^8.08)/y + t^8.47/y - t^8.54/y - t^3.99*y - t^4.98*y - 2*t^6.49*y - t^6.56*y - t^6.96*y - 2*t^7.48*y - 2*t^7.55*y - t^7.94*y + t^8.01*y + 2*t^8.08*y + t^8.47*y - t^8.54*y + t^8.97*y^2 | 2*g1*t^2.51 + g1^13*t^2.57 + t^2.97/g1^6 + t^3.49/g1 + 2*g1^11*t^3.56 + g1^4*t^4.02 + (2*t^4.48)/g1^3 + 2*g1^9*t^4.55 + 3*g1^2*t^5.01 + 2*g1^14*t^5.08 + g1^26*t^5.14 + (3*t^5.47)/g1^5 + 3*g1^7*t^5.54 + g1^19*t^5.61 + 4*g1^12*t^6.07 + 2*g1^24*t^6.13 + t^6.46/g1^7 + 5*g1^5*t^6.53 + 2*g1^17*t^6.59 - t^6.92/g1^14 + (3*t^6.99)/g1^2 + 6*g1^10*t^7.06 + 5*g1^22*t^7.12 + t^7.45/g1^9 + 5*g1^3*t^7.52 + 5*g1^15*t^7.58 + 3*g1^27*t^7.65 + g1^39*t^7.72 - t^7.91/g1^16 + (4*t^7.98)/g1^4 + 9*g1^8*t^8.04 + 8*g1^20*t^8.11 + g1^32*t^8.18 - t^8.44/g1^11 - g1*t^8.51 + 5*g1^13*t^8.57 + 4*g1^25*t^8.64 + 2*g1^37*t^8.7 + (3*t^8.97)/g1^6 + t^8.97/(g1^6*y^2) - t^3.99/(g1^2*y) - t^4.98/(g1^4*y) - (2*t^6.49)/(g1*y) - (g1^11*t^6.56)/y - t^6.96/(g1^8*y) - (2*t^7.48)/(g1^3*y) - (2*g1^9*t^7.55)/y - t^7.94/(g1^10*y) + (g1^2*t^8.01)/y + (2*g1^14*t^8.08)/y + t^8.47/(g1^5*y) - (g1^7*t^8.54)/y - (t^3.99*y)/g1^2 - (t^4.98*y)/g1^4 - (2*t^6.49*y)/g1 - g1^11*t^6.56*y - (t^6.96*y)/g1^8 - (2*t^7.48*y)/g1^3 - 2*g1^9*t^7.55*y - (t^7.94*y)/g1^10 + g1^2*t^8.01*y + 2*g1^14*t^8.08*y + (t^8.47*y)/g1^5 - g1^7*t^8.54*y + (t^8.97*y^2)/g1^6 |
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 |
|---|---|---|---|---|---|---|---|---|
| 61044 | ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }\phi_{1}q_{1}^{2}q_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{1}q_{1}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{1}$ | 1.3835 | 1.5679 | 0.8824 | [X:[1.3415], M:[0.8354, 1.1646], q:[0.6667, 0.3374], qb:[0.4979, 0.5226], phi:[0.3292]] | t^2.51 + t^2.58 + t^2.96 + 2*t^3.49 + 2*t^3.57 + t^4.02 + 2*t^4.48 + 2*t^4.56 + t^5.01 + t^5.09 + t^5.16 + 2*t^5.47 + 3*t^5.54 + t^5.62 - t^3.99/y - t^4.98/y - t^3.99*y - t^4.98*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 |
|---|---|---|---|---|---|---|---|---|---|
| 57693 | SU3adj1nf2 | ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }\phi_{1}q_{1}^{2}q_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{1}$ | 1.4621 | 1.6651 | 0.8781 | [X:[1.3424], M:[0.6976], q:[0.5746, 0.5219], qb:[0.4517, 0.479], phi:[0.3288]] | t^2.09 + t^2.92 + t^2.96 + t^3. + t^3.08 + t^3.16 + t^3.99 + t^4.03 + t^4.07 + t^4.15 + t^4.19 + t^4.89 + t^4.98 + t^5.01 + 2*t^5.05 + t^5.1 + 2*t^5.13 + t^5.17 + t^5.22 + t^5.25 + t^5.84 + t^5.88 + t^5.92 + t^5.96 - 2*t^6. - t^3.99/y - t^4.97/y - t^3.99*y - t^4.97*y | detail |