Landscape




$a$ =

$c$ =

$\leq a \leq$

$\leq c \leq$

id =





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.

#TheorySuperpotentialCentral charge $a$Central charge $c$Ratio $a/c$Matter field: $R$-chargeU(1) part of $F_{UV}$Rank of $F_{UV}$Rational
3946 SU2adj1nf2 $M_1q_1q_2$ + $ M_2\tilde{q}_1\tilde{q}_2$ + $ \phi_1q_1^2$ + $ M_1^2$ + $ M_3\phi_1q_2\tilde{q}_1$ + $ M_4q_1\tilde{q}_2$ + $ M_2M_5$ + $ M_6q_1\tilde{q}_1$ + $ M_6\phi_1q_2\tilde{q}_2$ + $ M_6M_7$ 0.6256 0.8117 0.7708 [X:[], M:[1.0, 0.9548, 0.7556, 0.7105, 1.0452, 0.7331, 1.2669], q:[0.7556, 0.2444], qb:[0.5113, 0.5339], phi:[0.4887]] [X:[], M:[[0], [-8], [1], [-7], [8], [-3], [3]], q:[[1], [-1]], qb:[[2], [6]], phi:[[-2]]] 1
Relevant OperatorsMarginal Operators$n_{marginal}$$-$$|F_{IR}|$Superconformal IndexRefined index
$M_4$, $ M_3$, $ q_2\tilde{q}_1$, $ q_2\tilde{q}_2$, $ \phi_1^2$, $ \phi_1q_2^2$, $ M_1$, $ M_5$, $ M_7$, $ \phi_1q_2\tilde{q}_2$, $ M_4^2$, $ M_3M_4$, $ M_4q_2\tilde{q}_1$, $ \phi_1q_1q_2$, $ M_4q_2\tilde{q}_2$, $ M_3^2$, $ M_3q_2\tilde{q}_1$, $ \phi_1\tilde{q}_1^2$, $ q_2^2\tilde{q}_1^2$, $ M_3q_2\tilde{q}_2$, $ \phi_1\tilde{q}_1\tilde{q}_2$, $ q_2^2\tilde{q}_1\tilde{q}_2$, $ \phi_1\tilde{q}_2^2$, $ q_2^2\tilde{q}_2^2$, $ M_4\phi_1^2$, $ M_4\phi_1q_2^2$, $ M_3\phi_1^2$, $ M_3\phi_1q_2^2$, $ \phi_1^2q_2\tilde{q}_1$, $ \phi_1q_2^3\tilde{q}_1$, $ M_1M_3$, $ M_4M_5$, $ \phi_1q_1\tilde{q}_1$, $ \phi_1^2q_2\tilde{q}_2$, $ \phi_1q_2^3\tilde{q}_2$, $ \phi_1q_1\tilde{q}_2$, $ M_3M_5$, $ M_5q_2\tilde{q}_1$, $ M_5q_2\tilde{q}_2$, $ \phi_1^4$, $ \phi_1^3q_2^2$, $ \phi_1^2q_2^4$, $ M_4M_7$, $ M_1\phi_1^2$, $ M_4\phi_1q_2\tilde{q}_2$ . -3 t^2.13 + 2*t^2.27 + t^2.33 + 2*t^2.93 + t^3. + t^3.14 + 2*t^3.8 + t^4.26 + 2*t^4.4 + t^4.47 + 4*t^4.53 + 3*t^4.6 + 2*t^4.67 + 2*t^5.06 + 3*t^5.2 + 5*t^5.27 + t^5.33 + 2*t^5.4 + t^5.47 + 3*t^5.86 + 2*t^5.93 - 3*t^6. + 4*t^6.07 + 2*t^6.14 + t^6.27 + t^6.39 + 2*t^6.53 + 2*t^6.67 + 4*t^6.73 + 6*t^6.8 + 3*t^6.87 + 6*t^6.94 + 2*t^7. + 2*t^7.2 + 3*t^7.33 + 2*t^7.4 + 3*t^7.47 + 6*t^7.53 + 7*t^7.6 + 4*t^7.67 + 2*t^7.74 + 2*t^7.8 + 3*t^8. + 6*t^8.2 - 6*t^8.27 + t^8.33 + 4*t^8.4 + 3*t^8.47 + t^8.53 + 2*t^8.54 + t^8.61 + 2*t^8.66 + 7*t^8.8 + 3*t^8.86 - 5*t^8.93 - t^4.47/y - t^6.6/y - t^6.73/y + t^7.4/y + t^7.47/y + (2*t^7.53)/y + (2*t^7.6)/y + (2*t^8.06)/y + t^8.13/y + (5*t^8.2)/y + (5*t^8.27)/y + (2*t^8.33)/y + (2*t^8.4)/y + t^8.47/y - t^8.73/y + (4*t^8.93)/y - t^4.47*y - t^6.6*y - t^6.73*y + t^7.4*y + t^7.47*y + 2*t^7.53*y + 2*t^7.6*y + 2*t^8.06*y + t^8.13*y + 5*t^8.2*y + 5*t^8.27*y + 2*t^8.33*y + 2*t^8.4*y + t^8.47*y - t^8.73*y + 4*t^8.93*y t^2.13/g1^7 + 2*g1*t^2.27 + g1^5*t^2.33 + (2*t^2.93)/g1^4 + t^3. + g1^8*t^3.14 + 2*g1^3*t^3.8 + t^4.26/g1^14 + (2*t^4.4)/g1^6 + t^4.47/g1^2 + 4*g1^2*t^4.53 + 3*g1^6*t^4.6 + 2*g1^10*t^4.67 + (2*t^5.06)/g1^11 + (3*t^5.2)/g1^3 + 5*g1*t^5.27 + g1^5*t^5.33 + 2*g1^9*t^5.4 + g1^13*t^5.47 + (3*t^5.86)/g1^8 + (2*t^5.93)/g1^4 - 3*t^6. + 4*g1^4*t^6.07 + 2*g1^8*t^6.14 + g1^16*t^6.27 + t^6.39/g1^21 + (2*t^6.53)/g1^13 + (2*t^6.67)/g1^5 + (4*t^6.73)/g1 + 6*g1^3*t^6.8 + 3*g1^7*t^6.87 + 6*g1^11*t^6.94 + 2*g1^15*t^7. + (2*t^7.2)/g1^18 + (3*t^7.33)/g1^10 + (2*t^7.4)/g1^6 + (3*t^7.47)/g1^2 + 6*g1^2*t^7.53 + 7*g1^6*t^7.6 + 4*g1^10*t^7.67 + 2*g1^14*t^7.74 + 2*g1^18*t^7.8 + (3*t^8.)/g1^15 + (6*t^8.2)/g1^3 - 6*g1*t^8.27 + g1^5*t^8.33 + 4*g1^9*t^8.4 + 3*g1^13*t^8.47 + t^8.53/g1^28 + 2*g1^17*t^8.54 + g1^21*t^8.61 + (2*t^8.66)/g1^20 + (7*t^8.8)/g1^12 + (3*t^8.86)/g1^8 - (5*t^8.93)/g1^4 - t^4.47/(g1^2*y) - t^6.6/(g1^9*y) - t^6.73/(g1*y) + t^7.4/(g1^6*y) + t^7.47/(g1^2*y) + (2*g1^2*t^7.53)/y + (2*g1^6*t^7.6)/y + (2*t^8.06)/(g1^11*y) + t^8.13/(g1^7*y) + (5*t^8.2)/(g1^3*y) + (5*g1*t^8.27)/y + (2*g1^5*t^8.33)/y + (2*g1^9*t^8.4)/y + (g1^13*t^8.47)/y - t^8.73/(g1^16*y) + (4*t^8.93)/(g1^4*y) - (t^4.47*y)/g1^2 - (t^6.6*y)/g1^9 - (t^6.73*y)/g1 + (t^7.4*y)/g1^6 + (t^7.47*y)/g1^2 + 2*g1^2*t^7.53*y + 2*g1^6*t^7.6*y + (2*t^8.06*y)/g1^11 + (t^8.13*y)/g1^7 + (5*t^8.2*y)/g1^3 + 5*g1*t^8.27*y + 2*g1^5*t^8.33*y + 2*g1^9*t^8.4*y + g1^13*t^8.47*y - (t^8.73*y)/g1^16 + (4*t^8.93*y)/g1^4


Deformation

Here is the data for the deformed fixed points from the chosen fixed point.

#SuperpotentialCentral Charge $a$ Central Charge $c$ Ratio $a/c$$R$-chargesSuperconformal IndexMore Info.Rational


Equivalent Fixed Points from Other Seed Theories

Here is a list of equivalent fixed points from other gauge theories.

#TheorySuperpotentialCentral Charge $a$ Central Charge $c$ Ratio $a/c$$R$-chargesSuperconformal IndexMore 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.

#TheorySuperpotentialCentral Charge $a$ Central Charge $c$ Ratio $a/c$$R$-chargesSuperconformal IndexMore Info.Rational
3680 SU2adj1nf2 $M_1q_1q_2$ + $ M_2\tilde{q}_1\tilde{q}_2$ + $ \phi_1q_1^2$ + $ M_1^2$ + $ M_3\phi_1q_2\tilde{q}_1$ + $ M_4q_1\tilde{q}_2$ + $ M_2M_5$ + $ M_6q_1\tilde{q}_1$ + $ M_6\phi_1q_2\tilde{q}_2$ 0.6454 0.8481 0.761 [X:[], M:[1.0, 0.9472, 0.7566, 0.7038, 1.0528, 0.7302], q:[0.7566, 0.2434], qb:[0.5132, 0.5396], phi:[0.4868]] t^2.11 + t^2.19 + 2*t^2.27 + t^2.35 + 2*t^2.92 + t^3. + t^3.16 + t^3.81 + t^4.22 + t^4.3 + 3*t^4.38 + 3*t^4.46 + 5*t^4.54 + 3*t^4.62 + 2*t^4.7 + 2*t^5.03 + 2*t^5.11 + 4*t^5.19 + 5*t^5.27 + 2*t^5.35 + 2*t^5.43 + t^5.51 + 3*t^5.84 + t^5.92 - 2*t^6. - t^4.46/y - t^4.46*y detail